• 한국세라믹학회지
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• 제36권2호
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• pp.203-209
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• 1999

Si 기판위에 Ba2YCu3O7-$\delta$ 고온초전도체를 응용하기 위해 요구되는 buffer층으로 유망한 재료인 LaAlO3 단일상 분말을 고상반응법과 자발착한 연소반응법으로 제조하였다. 제조된 LaAlO3 분말의 입자형태와 결정상태는 scanning electron microscope (SEM)과 X-ray diffractometer (XRD)를 이용하여 분석하였다. 분말의 비표면적과 소결특성은 각각 Brunauer-Emmett-Teller(BET) 방법과 dilatometer를 측정하였다. 고상반응법으로 LaAlO3 분말을 제조할 때에는 하소온도를 150$0^{\circ}C$까지 높게 하여도 단일상을 얻는 것이 어려웠으나 자발착한 연소반응법에 의한 분말제조는 $650^{\circ}C$의 저온에서 하소하여도 쉽게 얻을 수 있었다. Dilatometer 측정을 통하여 분석해 보면, 고상반응법에 의한 분말보다 자발착한 연소반응법에 의한 분말로 제조된 소결체가 고상반응법에 의한 소결체에 비해 1.4배나 큰 소멸밀도(98.87%)를 가졌다. 이렇게 소결밀도에서 큰 차이가 나는 것은 자발착한 연소방법에 의한 분말의 평균 입자크기가 nano crystal size이고 비표면적 값(56.54 $m^2$/g)이 매우 크기 때문이다. 두가지 방법으로 제조된 분말을 이용, LaAlO3 layer를 스크린 프린팅과 소결법으로 Si 기판상에 제조하였으며 자발착한 연소합성법으로 제조된 분말은 110$0^{\circ}C$에서 우수한 소결특성을 나타내었다.

• Applied Microscopy
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• 제25권4호
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• pp.124-131
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• 1995

이상과 같은 실험결과를 다음과 같은 요약할 수 있다. 1) $Hg_{1-x}\;Tl_{x}\;Ba_{2}(Ca_{0.86}\;Sr_{0.14})_{2}\;Cu_{3}\;O_{8+\delta}$의 구조는 Hg-1223과 같은 구조를 이루며 Hg 위치에 T1이 치환되어 있음을 알 수 있다. 2) 격자상수는 탈륨이 증가할수록 감소하는 경향을 나타냈으나 x=0.25 시료에서는 현저히 감소됨을 보였다. 3) x=0.25 시료에서는 적층 결함 1234구조가 1223구조와 intergrowth함을 보였고 불순물 상이 다소 나타났다. 4) 탈륨이 증가할 수록 보다 치밀하고 결함이 없는 안정된 조직을 보였다. 5) 모든 시료가 관찰 도중 전자빔에 대하여 손상되었으나 탈륨의 양이 증가할 수록 손상에 대한 저항이 커져 보다 안정된 상을 보였다.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2004년도 추계학술대회 논문집 전기설비전문위원
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• pp.93-96
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• 2004

In this paper, we analyzed the current limiting characteristics according to increase of source voltage in the flux-lock type high-Tc superconducting fault current limiter (SFCL). The flux-lock type SFCL consisted of two coils, which were wound in parallel each other through an iron core, and high-Tc superconducting (HTSC) element connected with coil 2 in series. The flux-lock type SFCL has the characteristics better in comparison with the resistive type SFCL because the fault current in the flux-lock type SFCL can be divided into two coils by the inductance ratio of coil 1 and coil 2. The fault current limiting operation of the flux-lock type SFCL can be different due to winding direction of the two coils. The winding method where the decrease of linkage flux between two coils in the accident happens is called the subtractive polarity winding and the winding method in case of the increase of linkage flux is called the additive polarity winding. The fault current limiting experiments according to the source voltage were performed for these two winding methods. Through the comparison and the analysis of the experimental data, we confirmed that the quench time was shorter, irrespective of the winding direction as the source voltage increased and that the fault current and the HTSC's resistance increased as the amplitude of the source voltage increased. The additive polarity winding made the fast quench time and the lower resistance of HTSC element in comparison with the subtractive polarity winding. The fault current of the subtractive polarity winding was larger than that of the additive polarity winding. In conclusion, we found that the additive polarity winding reduced the burden of SFCL because the quench time was shorter and the fault current was smaller than those of the subtractive polarity winding.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2009년도 춘계학술대회 논문집
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• pp.3-3
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• 2009

In order to investigate the possibility of using mixed rare earth $(Nd_{1/3}Eu_{1/3}Gd_{1/3})Ba_2Cu_3O_{7-x}$ (NEG123) as the superconducting layer of the HTS coated conductor, the NEG123 thin film was deposited epitaxialy on LAO(100) single crystal and IBAD_YSZ metal templates by pulsed laser deposition. Systematic studies were carried out to investigate the influences of deposition parameters of PLD on the micro structure, texture and superconducting properties of NEG-123 coated conductor. Deposition at oxygen partial pressure of 600 mTorr was needed to routinely obtain high quality NEG123 films with $J_c$'s (77K) over 2 MA/$cm^2$ and Tc's over 90K (${\Delta}T{\sim}2\;K$). We verified from magnetization study that the NEG123 has an improved in-field Jc as the field increases at temperatures between 10 K and 77 K compared with Gd123. The $J_c$ (77K, self field) and the value of onset $T_c$ of NEG123 thin film on LAO substrate was $4.0MA/cm^2$ and 92K, respectively. This is the first report, to the best of our knowledge, of coated conductors with NEG123 film as the superconducting layer which have Ic and Jc over 40 A/cm-width and 1.6 MA/$cm^2$ at 77K, self field. This study shows the possibility of using NEG123 film as the superconducting layer of the HTS coated conductor which can be used in high magnetic field power electric devices.