• 제목/요약/키워드: Bi-phase

검색결과 873건 처리시간 0.029초

Bi계 치환 고온 초전도체 (Studies of Element Substitution on Superconductivity in Bi-Sr-Ca-Cu-O Oxides)

  • 권오흥;박천제
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2000년도 추계학술대회 논문집
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    • pp.124-128
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    • 2000
  • The high Tc phase disappeared and low Tc phase increased in the substitution of transition elements for Bi ions. The high Tc phase decreased in the substitution of Si and Sn for Bi ions. The high Tc phase increased in the substitution of Sb, As and P which were the same group of Bi for Bi ions. The substitution of P ions was the most effective and then the high Tc phase was formed in large quantity by replacing Bi ions with 30% of P ions.

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

  • 양승호;박용필
    • 한국정보통신학회:학술대회논문집
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    • 한국해양정보통신학회 2007년도 춘계종합학술대회
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    • pp.536-539
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    • 2007
  • BSCCO 박막은 다양한 기판온도와 산화 가스압에 변화에서 증발법에 의해 제작되었다. 박막조성을 Bi2212 또는 Bi2223으로 설정했음에도 불구하고, 어느 경우나 Bi2201, Bi2212 및 Bi2223상이 생성되었다. 이들 안정상의 생성 영역은 기판 온도-산화 가스압의 Arrhenius 플롯에서 우측 하단 방향으로 경사진 직선으로 표시되며 매우 좁은 영역에 분포되어 있다. 생성막의 XRD 피크는 기판 온도에 따라 연속적으로 변화했다. 이는 Bi2201, Bi2212, Bi2223의 각상이 결정 구조 내에 혼합되어 있는 혼합 결정계의 존재를 나타내고 있으며, 각 상의 단상막은 매우 좁은 온도, 가스압 범위에서만 생성되었다.

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Influence of Sn/Bi doping on the phase change characteristics of $Ge_2Sb_2Te_5$

  • Park T.J.;Kang M.J.;Choi S.Y.
    • 정보저장시스템학회논문집
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    • 제1권1호
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    • pp.93-98
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    • 2005
  • Rewritable optical disk is one of the essential data storage media in these days, which takes advantage of the different optical properties in the amorphous and crystalline states of phase change materials. As well known, data transfer rate is one of the most important parameter of the phase change optical disks, which is mostly limited by the crystallization speed of recording media. Therefore, we doped Sn/Bi to $Ge_2Sb_2Te_5$ alloy in order to improve the crystallization speed and investigated the dependence of phase change characteristics on Sn/Bi doping concentration. The Sn/Bi doped $Ge_2Sb_2Te_5$ thin film was deposited by RF magnetron co-sputtering system and phase change characteristics were investigated by X-ray diffraction (XRD), static tester, UV-visible spectrophotometer, electron probe microanalysis (EPMA), inductively coupled plasma mass spectrometer (ICP-MS) and atomic force microscopy (AFM). Optimum doping concentration of Bi and Sn were 5${\~}$6 at.$\%$ and the minimum time for crystallization was below than 20 ns. This improvement is correlated with the simple crystalline structure of Sn/Bi doped $Ge_2Sb_2Te_5$ and the reduced activation barrier arising from Sn/Bi doping. The results indicate that Sn/Bi might play an important role in the transformation kinetics of phase change materials..

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The Influence of Bi-Sticking Coefficient in Bi-2212 Thin Film

  • Lee, Hee-Kab;Park, Yong-Pil;Lee, Joon-Ung
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2000년도 춘계학술대회 논문집 전자세라믹스 센서 및 박막재료 반도체재료 일렉트렛트 및 응용기술
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    • pp.152-156
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    • 2000
  • Bi-thin films are fabricated by an ion beam sputtering, and sticking coefficients of the respective elements are evaluated. The sticking coefficient of Bi element exhibits a characteristic temperature dependence : almost a constant value of 0.49 below $730^{\circ}C$ and decreases linearly with temperature over $730^{\circ}C$. This temperature dependence can be elucidated from the evaporation and sublimation rates of bismuth oxide, $Bi_2O_3$, from the film surface. It is considered that the liquid phase of the bismuth oxide plays an important role in the Bi(2212) phase formation in the co-deposition process.

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

  • 천민우;박용필;이성일
    • 한국전기전자재료학회논문지
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    • 제15권11호
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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/.

Bi2Sr2Ca2.2CuO3Ox계에서 초전도상과 Bi-free상의 핵생성과 성장 (Nucleation and Growth of Bi-free and Superconducting Phases in Bi2Sr2Ca2.2CuO3Ox)

  • 오용택;신동찬;구재본;이인환;한상철;성태현
    • 한국전기전자재료학회논문지
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    • 제16권4호
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    • pp.343-350
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    • 2003
  • Using Bi$_2$Sr$_2$Ca$_2$.$_2$Cu$_3$ $O_{x}$ powders prepared by solid state reaction and spray drying method, the nucleation and growth behaviors of superconducting and second phases were investigated during isothermal heat treatment. When the spray drying power was used in contrast with solid state reaction powder, Bi$_2$Sr$_2$Ca$_2$.$_2$Cu$_3$ $O_{x}$ (2223) phase could be formed at the relatively shot time and second phases were much bigger. Quantitative analysis showed that as the heat treatment time increased, more Bi$_2$Sr$_2$Ca$_2$.$_2$Cu$_3$ $O_{x}$ (2212) changed to 2223 and the major second phase was changed from (Sr,Ca)$_{14}$Cu$_{24}$ $O_{x}$(14:24) to (Sr,Ca)$_2$Cu$_1$ $O_{x}$ (2:l). The superconducting phase formed at the relatively short time 14:24 phase. Following the Bi-free phase of 14:24 Phase, but long time was needed in places far from the 14:24 phase. Following the formation of the 2212 phase near the 14:24 phase, the 2223 phase nucleated preferentially at the interface between the 2212 and 14:24 phases. The preferential nuclcation of 2223 was explained by its structural similarity and low Interfacial energy with both the Bi-free and 2212 Phases.12 Phases.

동피복재법을 이용한 Bi-Sr-Ca-Cu-O 고온초전도 후막 제조 (Fabrication of Cu-Sheathed Bi-Sr-Cu-O High Temperature Superconductor Thick Films)

  • 한상철;성태현;한영희;이준성;정상진
    • 한국초전도저온공학회:학술대회논문집
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    • 한국초전도저온공학회 1999년도 제1회 학술대회논문집(KIASC 1st conference 99)
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    • pp.22-25
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    • 1999
  • A well oriented Bi-2212 superconductor thick films were fabricated by screen printing with a Cu-free Bi-Sr-Ca-Cu-O powder on a copper plate and heat-treating at 820- $880^{\circ}C$for several minute in low oxygen pressure or are. At minute in low oxygen pressure of air. At , the printing layer partially melted by reaction between the Cu-free precursor by reaction between the Cu-free$870^{\circ}C$ precursor and CuO of the oxidizing copper plate. It is believed that the solid phase is Bi : Sr : Ca : Cu = 2 : 2 : 0 : 1. It is likely that the Bi-2212 superconducting phase is formed at Bi-2212 superconducting phase is formed at Bi-free phase/liquid interface by nucleation and grows.

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Analysis of Bi-Superconducting Thin Films Fabricated by Using the Layer by Layer Deposition and Evaporation Deposition Method

  • Yang, Seung-Ho;Cheon, Min-Woo;Lee, Ho-Shik;Park, Yong-Pil
    • 한국정보통신학회:학술대회논문집
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    • 한국해양정보통신학회 2007년도 춘계종합학술대회
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    • pp.517-520
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    • 2007
  • The BSCCO thin film fabricated by using the layer by layer deposition method was compared with the BSCCO thin film fabricated by using the evaporation method. Reevaporation in the form of Bi atoms or $Bi_2O_3$molecules easily bring out the deficiency of Bi atoms in thin film due to the long sputtering time of the layer by layer deposition. On the other hand, the respective atom numbers corresponding to BSCCO phase is concurrently supplied on the film surface in the evaporation deposition process and leads to BSCCO phase formation. Also, it is cofirmed that by optimizing the deposition condition, each single phase of the Bi2201 phase and the Bi2212 phase can be fabricated, the sticking coefficient of Bi element is clearly related to the changing of substrate temperature and the formation of the Bi2212 phase.

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Phase Transformation of Sn-Pb-Bi Solder for Photovoltaic Ribbon: A Real-time Synchrotron X-ray Scattering Study

  • Cho, Tae-Sik
    • Transactions on Electrical and Electronic Materials
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    • 제15권3호
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    • pp.155-158
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    • 2014
  • The phase transformation of Sn-Pb-Bi solder for photovoltaic ribbon during soldering was studied using real-time synchrotron x-ray scattering. At room temperature, Sn and Pb crystal phases in the solder existed separately. By heating to $92^{\circ}C$, a new PbBi alloy crystal phase was formed, which grew further up to $160^{\circ}C$. The Sn crystal phase first started to melt at $160^{\circ}C$, and was mostly melted at $165^{\circ}C$. In contrast, the Pb and PbBi crystal phases started to melt at $165^{\circ}C$, and were mostly melted at $170^{\circ}C$. The useful result was obtained, that the solder's melting temperature decreased from $183^{\circ}C$ to $170^{\circ}C$ by addition of a small amount of Bi atoms to the eutectic Sn62-Pb38 (wt%) solder. Our study first revealed the detailed in-situ phase transformation of Sn-Pb-Bi solder during heating to the eutectic temperature. Considering the results of peel strength and hardness, adding 1 wt% of Bi atoms to the Sn62-Pb38 (wt%) solder produced an appropriate composition.

스퍼터링 법과 증발 법으로 제작한 초전도 박막의 비교 (Comparison between Superconducting Thin Films Fabricated by Using the Sputtering and the Evaporation Method)

  • 천민우;박노봉;양승호;박용필;김혜정
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2004년도 제6회 학술대회 논문집 일렉트렛트 및 응용기술연구회
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    • pp.39-42
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    • 2004
  • The $Bi_2Sr_2Ca_nCu_{n+1}O_x$ superconducting thin film fabricated by using the sputtering method was compared with the $Bi_2Sr_2Ca_nCu_{n+1}O_x$ superconducting thin film fabricated by using the evaporation method. In doing the ultra-low deposition because each element can exist on the substrate surface, both the sputtering method and the evaporation method could easily fabricate single phase of the Bi2212 phase. Also, it is cofirmed that by optimizing the deposition condition, each single phase of the Bi2201 phase and the Bi2212 phase can be fabricated, the sticking coefficient of Bi element is clearly related to the changing of substrate temperature and the formation of the Bi2212 phase.

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