• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1992년도 춘계학술대회 논문집
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• pp.64-69
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• 1992

Bi-Sr-Ca-Cu-O superconducting system have the low and high Tc phases. In order to get the superconductor above crtitical temperature 100K, we added with Pb and sintered for a long time about 200 hrs. In this study, the influence of superconducting characteristics on the Bi(Pb)SrCaCuO system characteristics on the Bi(Pb)SrCaCuO system dopped Sb was investigate too. Adding Sb of 0.1 mol, the sintering time is short than that dopped Pb only. We could get the critical temperature 102 K at sintered for 24 hrs and 109 K for 210 hrs.

• 전기학회논문지
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• 제59권1호
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• pp.120-122
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• 2010

In this paper the effect of constituent content on superconductivity and phase in BiPbSrCaCuO system was reported. The zero resistance temperature reaches as high as 100k when dophant Sb was decreased dramatically with increasing Sb content in BiPbSrCaCuO system while the corresponding phase was changed fundamentally.

• 한국재료학회지
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• 제6권7호
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• pp.684-691
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• 1996

Bi-계 고온초전도체인 Bi2Sr2Ca2Cu3O10(Bi-2223)단일상을 반응시간을 줄이면서 합성하기 위하여 Bi-Sr-Ca-Cu-O계 내에 존재하는 Bi2Sr2Ca2Cu3O10(Bi-22o1), Bi2Sr2Ca2Cu3O10(Bi-2212), (Ca0.91Sr0.09)-CuO2의 혼합물, 특히 정확한 Bi1.7Pb0.4Sr2Ca2Cu3O10+x의 조성대신 (Ca0.91Sr0.09)CuO2가 많이 첨가된 조성의 혼합물에서 Bi-2223가 가장 쉽게 형성되었다. Bi-2223상은 86$0^{\circ}C$와 87$0^{\circ}C$에서 60시간 이내에 형성되었다. 소량의 Bi-2212상은 장시간의 반응후에도 여전히 존재하였다. 중간화합물을 이용한 합성방법이 통상의 소결방법에 비해 반응시간내에 소량의 불순물상들을 가진 Bi-2223상을 형성시킬 수 있다.

• 대한전기학회논문지
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• 제41권7호
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• pp.766-772
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• 1992

Bi-Sr-Ca-Cu-O superconducting system has both the low and high Tc phases. We added Pb and sintered for 200hrs. in OS12T atmosphere in order to get the superconductor above critical temperature 100K. Superconducting properties of the Bi(Pb)SrCaCuO system doped Sb were also investigated. When Sb of 0.1mol is added, the sintering time becomes shorter than that doped Pb only. We could get the critical temperature 102K at the samples sintered for 24hrs. and 109K for 210hrs.

• 한국전기전자재료학회논문지
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• 제16권5호
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• pp.429-434
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• 2003

The magnetic field sensor was fabricated with superconducting ceramics of BiPbSrCaCuO system. The sensor at liquid nitrogen temperature showed the increase of electrical resistance by applying magnetic field. Actually, the voltage drop across the sensor was changed from zero to a value more than 100 $\mu\textrm{V}$ by the applied magnetic field. The change of electrical resistance depended on magnetic field. The sensitivity of this sensor was 2.9 $\Omega$/T. The sensing limit was about 1.5${\times}$10$\^$-5/ T. The increase of electrical resistance by the magnetic field was ascribed to a modification of the Josephson junctions due to the penetrating magnetic flux into the superconducting material. Considering the observed properties of the superconductor with trapped magnetic flux, a magnetic sensor was fabricated to detect simultaneously both the intensity and the direction of the magnetic field.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1991년도 추계학술대회 논문집 학회본부
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• pp.269-273
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• 1991

High Tc oxide superconductor with a Tc above 100 K has been successfully prepared by solid state reaction method in added-Pb BiSrCaCuO system. As compared with 123 compound, the formation reaction of the high Tc requires long time heat treatment. It is due to the transformation from the low Tc phase to high Tc phase. The sintering just below the melting point of the calcined powder mixture is effective on the formation of the high Tc phase in BiSrCaCuO system to be added with Pb. The growth of the high Tc superconducting phase has a thin plate shape, which is characterized by the c parameter of 37${\AA}$. The formation kinetics is also investigated in the samples with different Bi/Pb ratio and the 30% Pb addition is most preferable for the formation of the high Tc phase. The formation of the high Tc phases is delayed by the excessive addition of Pb. The lattice parameter(c) of the unit cell(both the low and high Tc phases) is increased with increase of Pb.

• 한국재료학회지
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• 제1권2호
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• pp.71-76
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• 1991

The superconducting powders in $YBa_2Cu_3O_{7-x}$ and Bi-Pb-Sr-Ca-Cu-O system were easily prepared from water in oil type emulsion by loading each cation into the aqueous phase. In $YBa_2Cu_3O_{7-x}$ system, the superconducting orthorhombic phase was formed by calcining at $750^{\circ}C$ for 10h in $O_2$. The size of the superconducting phase powders was submicron. The density of the sintered specimen using this powders was about 95% of the theoretical density and the resistance sharply decreases at about 90K, In Bi-Pb-Sr-Ca-Cu-O system the low Tc phase($(Bi, Pb)_2Sr_2Ca_1Cu_2O_y$) was formed by calcining at $800^{\circ}C$ for 10h in a low oxygen partial pressure of 1/20 atm The shape of clacined powder is thin plate of which size is about $2\mu\textrm{m}$ and thickness is smaller than $\mu\textrm{m}$. It was observed that the high Tc phase ($(Bi, Pb)_2Sr_2Ca_2Cu_3O_y$) was formed by sintering at $850^{\circ}C$ for 30h in oxygen pressure of 1/20 atm without intermediary grinding. The above sintered sample exhibited superconductivity with a Tc(zero)=105K.

• E2M - 전기 전자와 첨단 소재
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• 제4권4호
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• pp.293-303
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• 1991

소결 후 냉각 및 Annealing이 Bi(Pb)SrCaCuO계 초전도체의 특성에 미치는 영향에 대해 연구하였다. 소결 후 시편을 500[.deg.C]에서 5[hr] Annealing함으로써 1)미세조직이 치밀화 되었으며 고온상의 체적비가 증가하였다. 2)임계온도 및 전류밀도 특성이 향상되었다.

• 전기학회논문지
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• 제59권2호
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• pp.352-354
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• 2010

The effects of Au addition on the structure and the superconducting properties of Bi system bulk have been investigated. Au exists in the metalic form in above materials. It does not affect the formation and structure of the BiSrCaCuO(2223) phase. The superconducting transition temperature Tc does not change for $Bi_{1.7}Pb_{0.3}Sr_2Ca_2Cu_3O$ composite However Au doping can make the grains smaller. Metallic Au can make gathers on the grains boundary and lead to the increment of critical transport current density. The current density of $Bi_{1.7}Pb_{0.3}Sr_2Ca_2Cu_3Au_{0.5}O$ was 1000A/$cm^2$ at liquid nitrogen temperature.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1992년도 하계학술대회 논문집 B
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• pp.740-743
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• 1992

Effects of powder sintering and 2nd, pressing on the superconducting characteristics in the (Bi,Pb)SrCaCuO system have been studied. The sample prepared by the powder sintering process had a porous microstructure with a $T_c$ below 77 K, while the sample prepared by 2nd. pressing process had highly oriented microstructure with a $T_c$ above 100 K. The critical current density($J_c$) was relatively improved in the sample prepared by the 2nd. pressing process. But the value of $J_c$ is cosiderably low in practical use.