• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1999년도 추계학술대회 논문집
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• pp.69-72
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• 1999

A Well oriented Bi$_2$re$_2$CaCu$_2$O$\sub$8/(Bi2212) superconductor thick films were formed successfully on a copper substrate by liquid reaction between a Cu-free precursor and Cu tape using method in which Cu-free BSCO powder mixture was printed on copper plate and heat-treated. And we examined the mechanism for the rapid formation of Bi2212 superconducting films from observing the surface microstructure with heat-treatment time. At heat-treatment temperature, the printing layer partially melt by reacting with CuO of the oxidizing copper plate, and the nonsuperconducting phases present in the melt are typically Bi-free phases and Cu-free phases. Following the partial melting, the Bi$_2$Sr$_2$CaCu$_2$O$\sub$8/ superconducting phase is formed at Bi-free phase/liquid interface by nucleation and grows. It was confirmed that the phase colony from the phase diagram of Bi$_2$O$_3$-(SrO+CaO)/2-CuO system is similar to the observed result.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2002년도 추계학술대회 논문집 Vol.15
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• pp.276-279
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• 2002

$Bi_{2}Sr_{2}CaCu_{2}O_{x}$ was prepared by the conventional method of solid state reaction and SHS method. The samples were annealed in different atmosphere in order to examine the influence of atmospheres on the carbon contents in the $Bi_{2}Sr_{2}CaCu_{2}O_{x}$ compound. The lowest carbon content in $Bi_{2}Sr_{2}CaCu_{2}O_{x}$ could be attended when the sample was annealed in $O_{2}$ at $800^{\circ}C$ for 100 hours. The $CO_{2}$ in air pollute the samples and increase the carbon content in the sintering process. The critical current density of the $Bi_{2}Sr_{2}CaCu_{2}O_{x}$ samples will decrease with the increasing carbon contents in the samples. The impurity carbon will deposit in the grain boundary, which makes critical current density lower.

• 한국초전도저온공학회:학술대회논문집
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• 한국초전도저온공학회 1999년도 제1회 학술대회논문집(KIASC 1st conference 99)
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• pp.47-50
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• 1999

The orientation mechanism of an amorphous $Bi_{2}$$Sr_{2}$$Ca_{2 x}$$Cd_{x}$$Cu_{3}$$O_{y}$ phase were studied by using the dilatometry. The amorphous $Bi_{2}$$Sr_{2}$$Ca_{2 x}$$Cd_{x}$$Cu_{3}$$O_{y}$ samples brought about a volume shrinkage at the onset of the crystallization of a $Bi_{2}$$Sr_{2}$$CaCu_{2}$$O_{6}$phase around $400^{\circ}C$. The random crystal growth of $Bi_{2}$$Sr_{2}$$CaCu_{2}$$O_{8}$ phase around $800^{\circ}C$. yielded a rapid volume expansion and after then samples shrinmed, accompanied with the crystal orientation. The$Bi_{2}$$Sr_{2}$$Ca_{2 x}$$Cd_{x}$$Cu_{3}$$O_{y}$ (x=0.4) sample exhibited the best-oriented structure because the liquid phase formed seemed to have the lowest viscosity which would contributed to the easy collapse of the card-house structure.

• 한국정보통신학회:학술대회논문집
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• 한국해양정보통신학회 2007년도 춘계종합학술대회
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• pp.524-527
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• 2007

이온 빔 스퍼터법을 이용하여 저속성장으로 동시 증착에 의해 $Bi_2Sr_2Ca_{n-1}Cu_nO_x$(n=0, 1, 2) 박막을 제작하였다. Bi 2212 상은 기판온도 $750\sim795^{\circ}C$의 범위에서 나타났으며, $750^{\circ}C$보다 저온 측에서는 Bi 2201의 단일강이 존재하였나. 그러나, 조성과 관계되는 $PO_3$에 대해서 크게 변하지 않았다. 그리고 임계온도(Tc)가 $45\sim90K$ 가지는 c축 배향한 고품질의 Bi 2212 박막을 얻었다. 소수의 박막에서는 소량의 CuO가 불순물로 관찰되었으며, 얻어진 모든 박막에서 $CaCuO_2$의 불순물 상은 관찰되지 않았다.

• 한국정보통신학회논문지
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• 제11권6호
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• pp.1115-1121
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• 2007

이온 빔 스퍼터법을 이용하여 저속성장으로 동시 증착에 의해 $Bi_2Sr_2Ca{_{n-1}}Cu_nO_x$(n=0,1,2) 박막을 제작하였다. Bi 2212 상은 기판온도 $750{\sim}795^{\circ}C$의 범위에서 나타났으며, $750^{\circ}C$보다 저온 측에서는 Bi 2201의 단일상이 존재하였다. 그러나, 조성과 관계되는 $PO_3$은 압력 변화에 대해서는 관찰되지 않았다. 그리고 $45{\sim}90K$의 임계온도(Tc)를 갖는 c축 배향한 고품질의 Bi 2212 박막을 얻었다. 소수의 박막에서는 소량의 CuO가 불순물로 관찰되었으며, 얻어진 모든 박막에서 $CaCuO_2$ 의 불순물 상은 관찰되지 않았다.

• 대한전기학회논문지
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• 제43권5호
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• pp.795-801
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• 1994

The BiPbSrCaCuO superconductor was fabricated by diffusion of The dual layer composed of SrS12TCaS11TCuS12TOS1xT in upper layer and BiS12TPbSI0.3TCuS12TOS1yT in lower layer, and varified growh-mechanism of BiPbSrCaCuO superconducting phase. And, we produced optimum conditions of spread volume and each stage of sintering time were upper layer:Lower layer=1:0.2, 1:0.4, 1:0.6 and 24hr., 120hr., 210hr. From the result, the optimum conditions are spread volume(Upper layer:Lower layer=1:0.6), sintering time(210hrs.) at 820$^{\circ}C$.The BiPbSrCaCuO superconductor, fabricated optimum condition, showed zero resistance at critical temperature of 70k.

• 한국전기전자재료학회논문지
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• 제18권5호
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• pp.464-467
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• 2005

BiSrCaCuO superconducting ceramic thick films were fabricated by chemical process. The x ray diffraction pattern of the BiSrCaCuO thick films contained 110 K phase. The critical temperature of BiSrCaCuO thick films were Tc=95 K-97 K. The critical temperature and critical density of BiSrCaCuO thick film grown at $750 {\circ}C$ were Tc = 95 K and $Jc= 7{\times}10^{6} A/cm^{2}$ We obtained high-Jc as-grown BiSrCaCuO on an MgO substrate by low fressure CVD.

• 대한전기학회논문지:전기물성ㆍ응용부문C
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• 제52권6호
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• pp.249-256
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• 2003

Samples with the nominal composition, Ag-$Bi_{1.84}Pb_{0.34}Sr_{1.91}Ca_{2.03}Cu_{3.06}O_{10+{\delta}}$ high $T_{c}$ superconductors containing Ag as an additive were fabricated by a solid-state reaction method. Samples with Ag of 10 wt%, 30 wt%, and 50 wt% each were sintered at $860^{\circ}C$~$870^{\circ}C$ for 24 hours. The structural characteristics, the microstructures and the critical temperature with respect to the each samples were investigated by XRD, four-prove methode, SEM and EDS respectively. The $T_{c}\;^{zero}$ of the sample with the 50 wt% Ag additive at the surface showed 94 K.

• 대한용접접합학회:학술대회논문집
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• 대한용접접합학회 2005년도 추계학술발표대회 개요집
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• pp.262-264
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• 2005

$Bi_{2}Sr_{2}CaCu_{2}O_{x}$(Bi-2212) and $Bi_{2}Sr_{2}Ca_{2}Cu_{3}O_{y}$(Bi-2223) high-$T_{c}$ superconductor(HTS) coating have been prepared by plasma spraying and heaat treatment. The Bi-2212 HTS coating later is synthesized through the peritectic reaction between Sr-Ca-Cu oxide coating layer and Bi-Cu oxide coating later, and $Bi_{2}Sr_{2}CaCu_{2}O_{y}$(Bi-2212) superconducting phase grow by partial melting process. The superconducting characteristic depends strongly on the conditions of the partial melting process. the Bi-2212 HTS layer consists of the whiskers grown in the diffusion direction. Above the 2212 layer, Bi-2223 phase and secondary phase was observed. The secondary phase is distributed uniformly over the whole surface. This is caused to the microcrack on the coatings surface. Despite everything, the film shows superconducting with an onset $T_{c}$ of about 115K. There are two changes steps. One changes (1step) at 115K is due to the diamagnetism of the Bi-2223 phase and the other changes (2step) at 78K is due to the diamagnetism of the Bi-2212 phase.

• 공업화학
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• 제16권2호
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• pp.296-303
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• 2005

PVC와 ABC의 혼합물을 대상으로 혼합비에 따른 공열분해 특성과 CaO와 $Cu_2O$의 첨가효과를 TG와 GC-MS를 이용하여 연구하였다. $500^{\circ}C$의 등온실험에서 ABS의 혼합비율이 증가할수록 스티렌 단량체와 방향족 화합물의 수율은 증가하였으며, BTX 화합물의 최대 수율은 PVC와 ABS의 혼합비가 4:1일 때 16.14% 정도임을 확인하였다. 금속산화물을 첨가한 경우 액상 생성물의 수율은 혼합비 0.4의 CaO를 첨가했을 때 73%와 0.4의 $Cu_2O$를 첨가했을 때 70%인 최대값을 얻을 수 있었으며, 각각 혼합비 0.5인 CaO와 1.0인 $Cu_2O$를 첨가했을 때 기상 생성물에 포함된 염화수소를 완전히 제거할 수 있었다. 본 연구의 실험조건에서는 염화수소를 완전히 제거할 수 있고, 가장 높은 액상 수율을 얻을 수 있는 반응조건은 $500^{\circ}C$에서 혼합비 0.5인 CaO나 혼합비 1.0인 $Cu_2O$를 첨가하는 것으로 사료된다.