• Title/Summary/Keyword: BSCCO(2201)

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Layer-by-layer Deposition of BSCCO Thin Films Using Ion Beam Sputtering Method (이온 빔 스퍼터법에 의한 BSCCO 박막의 순차 증착)

  • 박용필;이준웅
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.11 no.4
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    • pp.334-339
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    • 1998
  • $Bi_2Sr_2CuO_x$(Bi-2201) thin films have been fabricated by atomic layer-by-layer deposition using ion beam sputtering (IBS) method. During the deposition, 14 wt%-ozone/oxygen mixture gas of typical pressure of $5.0\times10^{-5}$ Torr is supplied with ultraviolent light irradiation for oxidation. XRD and RHEED investigations reveal that a buffer layer with compositions different from Bi-2201 is formed at the early deposition stage of less than 10 units cell and then Bi-2201 oriented along the c-axis is grown.

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Epitaxial Growth of BSCCO Films by IBS Method (IBS법에 의한 BSCCO 박막의 에피택셜 성장)

  • 양승호;박용필
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2002.05a
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    • pp.627-630
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    • 2002
  • Bi$_2$Sr$_2$CuOx(Bi-2201) thin films were fabricated by atomic layer-by-layer deposition using an ion bean sputtering method. 10 wt% and 90 wt% ozone mired with oxygen were used with ultraviolet light irradiation to assist oxidation. XRD and RHEED investigations revealed that a buffer layer is formed at the early stage of deposition (less than 10 unit cell), and then c-axis oriented Bi-2201 grows on top of it.

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Analysis of Sticking Coefficient in BSCCO Thin Film (BSCCO 박막의 부착계수 해석)

  • Chun, Min-Woo;Park, Yong-Pil
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.11a
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    • pp.252-255
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    • 2002
  • BSCCO thin films are fabricated by an ion beam sputtering method, and sticking coefficients of the respective elements are evaluated. The sticking coefficient of Bi element in BSCCO film formation was observed to show a unique temperature dependence; it was almost a constant value of 0.49 below about $730^{\circ}C$ and decreased linearly over about $730^{\circ}C$. In contrast, Sr and Ca, displayed no such remarkable temperature dependence. This behavior of the sticking coefficient was explained consistently on the basis of the evaporation and sublimation processes of $Bi_{2}O_{3}$. It was concluded that Bi(2212) thin film constructs from the partial melted Bi(2201) phase with the aid of the liquid phase of $Bi_{2}O_{3}$.

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R-T Characteristic in BSCCO Thin Films (BSCCO 박막의 저항-온도 특성)

  • Cheon, Min-Woo;Yang, Sung-Ho;Park, Yong-Pil
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2005.05b
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    • pp.98-101
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    • 2005
  • BSCCO thin films fabricated by using the evaporation method. As a result, although the composition of Bi2212 was set up, the phase of Bi2201, Bi2212 and Bi2223 was formed. The formation area of these stable phases is indicated as inclined line in the direction of the right lower end from the Arrhenius plot of the substrate temperature-oxidation gas pressure, and are distributed in very small area. The activation energy for the phase transformation from the Bi2201 to the Bi2212 is estimated in terms of the Avrami equation.

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A Study on Produced Region of Bi-2223 Superconducting Thin Films versus substrate temperature and oxide gas pressures for formation of single-phase Film (단상막 형성을 위해 기판온도와 산화 가스압에 따른 Bi-2223 초전도 박막의 생성 영역에 관한 연구)

  • Yang, Seung-Ho;Park, Yong-Pil
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2007.06a
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    • pp.536-539
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    • 2007
  • BSCCO am films fabricated by using the evaporation method at various substrate temperatures, Tsub and ozone gas pressures $PO_3$. Despite setting the composition of thin film Bi2223, Bi2201, Bi2212 and Bi2223 phase were appeared. It was confirmed the obtained field of stabilizing phase was represented in the diagonal direction of the right below end in the Arrhenius plot of temperature of the substrate and $PO_3$, and it was distributed in the rezone. The XRD peak of the generated film continuously changed according to the substrate temperature. This demonstrates the existence of mixed crystal composition where the phases of Bi2201, Bi2212 and Bi2223 are mixed in the crystal structure; and the single-phase film of each phase exist in a very rezone of temperature and gas pressure.

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Epitaxial Growth of BSCCO Type Structure in Atomic Layer by Layer Deposition

  • Yang, Sung-Ho;Park, Yong-Pil;Jang, Kyung-Uk;Oh, Geum-Gon;Lee, Joon-Ung
    • Proceedings of the Korean Institute of Navigation and Port Research Conference
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    • 2000.11a
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    • pp.97-100
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    • 2000
  • Si$_2$Sr$_2$CuO$\sub$x/(Bi(2201)) thin films are fabricated by atomic layer by layer deposition using ion beam sputtering(IBS) method. During the deposition, 10 %-ozone/oxygen mixture gas of typical 5.0 ${\times}$ 10$\^$-5/ Torr is applied with ultraviolet light irradiation for oxidation. XRD and RHEED investigations reveal out that a buffer layer with some different compositions is formed at the early deposition stage of less than 10 units cell and then c-axis oriented Bi(2201) is grown.

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Epitaxial Growth of BSCCO Films by Leyer-by-Layer Deposition (순차 증착에 의한 BSCCO 박막의 에피택셜 성장)

  • 안준호;박용필;김정호
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.14 no.10
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    • pp.855-860
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    • 2001
  • Bi$_2$Sr$_2$CuO$_{x}$(Bi-2201) thin film were fabricated by atomic layer-by -layer deposition using an ion beam sputtering method. 10 wt% and 90 wt% ozone mixed oxygen were used with ultraviolet light irradiation to assist oxidation. XRD and RHEED investigations revealed that a buffer layer is formed at the early stage of deposition (less than 10 unit cell), and then c-axis oriented Bi-2201 grows on top of it.t.

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Epitaxial Growth of BSCCO Type Structure in Atomic Layer by Layer Deposition

  • Yang, Sung-Ho;Park, Yong-Pil;Jang, Kyung-Uk;Oh, Geum-Gon;Lee, Joon-Ung
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.11a
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    • pp.97-100
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    • 2000
  • Bi$_2$Sr$_2$CuO$\sub$x/(Bi(2201)) thin films are fabricated by atomic layer by layer deposition using ion beam sputtering(IBS) method. During the deposition, 10 %-ozone/oxygen mixture gas of typical 5.0 ${\times}$ 10$\^$-5/. Torr is applied with ultraviolet light irradiation for oxidation. XRD and RHEED investigations reveal out that a buffer layer with some different compositions is formed at the early deposition stage of less than 10 units cell and then c-axis oriented Bi(2201) is grown.

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Analysis of Sticking Coefficient in Bi-Superconducting Thin film (Bi 초전도 박막의 부착계수 해석)

  • 천민우;박용필;이성일
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.15 no.11
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    • pp.997-1002
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    • 2002
  • BSCCO thin films are fabricated by an ion beam sputtering method, and sticking coefficients of the respective elements are evaluated. The sticking coefficient of Bi element in BSCCO film formation was observed to show a unique temperature dependence; it was almost a constant value of 0.49 below about 730$^{\circ}C$ and decreased linearly over about 730$^{\circ}C$ In contrast, Sr and Ca, displayed no such remarkable temperature dependence. This behavior of the sticking coefficient was explained consistently on the basis of the evaporation and sublimation processes of Bi$\sub$2/O$\sub$3/. It was concluded that Bi(2212) thin film constructs from the partial melted Bi(2201) phase with the aid of the liquid phase of Bi$\sub$2/O$\sub$3/.

Analysis of Sticking Coefficient in BSCCO Thin Film Fabricatied for apply to Biomedical device (의용소자로 응용하기 위해 제작한 BSCCO 박막의 부착계수 해석)

  • Yang, Seung-Ho;Park, Yong-Pil
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2006.11a
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    • pp.351-352
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    • 2006
  • BSCCO thin films are fabricated by an ion beam sputtering method, and sticking coefficients of the respective elements are evaluated. The sticking coefficient of Bi element in BSCCO film formation was observed to show a unique temperature dependence; it was almost a constant value of 0.49 below about $730^{\circ}C$ and decreased linearly over about $730^{\circ}C$. In contrast, Sr and Ca, displayed no such remarkable temperature dependence. This behavior of the sticking coefficient was explained consistently on the basis of the evaporation and sublimation processes of $Bi_2O_3$. It was concluded that Bi(2212) thin film constructs from the partial melted Bi(2201) phase with the aid of the liquid phase of $Bi_2O_3$.

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