• 대한전기학회논문지:전기물성ㆍ응용부문C
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• 제52권6호
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• pp.241-248
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• 2003

$Bi_{1.84}Pb_{0.34}Sr_{1.91}Ca_{2.03}Cu_{3.06}O_{10+\delta}$ high $T_{c}$ superconductors containing Ag as an additive were fabricated by a solid-state reaction method. The superconducting properties, such as the structural characteristics, the critical temperatures, the grain size and the image of mapping on the surface were investigated. Samples with Ag and Au of 50 wt% each were sintered at various temperature(820~$850^{\circ}C$). The structural characteristics, the microstructure of surface and the critical temperature with respect to the each samples were analyzed by XRD and SEM, EDS and four-prove methode respectively. The critical temperature showed the result which the Ag additive samples are higher than Au additive samples. The microstructure of the surface showed the tendency which the Ag additive samples become more minuteness than Au additive samples.

• 한국세라믹학회지
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• 제40권6호
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• pp.530-538
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• 2003

110 K 상의 산화물 고온초전도체를 B $i_{1.84}$P $b_{0.34}$S $r_{1.91}$C $a_{2.03}$C $u_{3.06}$ $O_{10+}$$\delta$의 출발조성비로 고상반응법에 의해 합성하였다. 합성된 Bi계 110 K 상의 산화물 고온초전도 물질을 다시 분말 상태로 만든 후, MgO 금속산화물 분말을 5~50 wt%의 각 비율로 혼합하였다. MgO 금속산화물 분말이 혼합된 시편들을 820~86$0^{\circ}C$로 24시간동안 최종 소결시켰다. 그 후, 각 시편들에 대하여 x-선, $T_{c}$, SEM 등을 측정하여 MgO 금속산화물 혼합량에 대한 초전도특성 및 표면의 입자 크기 변화 등에 대한 조사를 진행하였다. MgO 금속산화물의 혼합량이 증가됨에 따라 MgO 관련 피크들의 강도 및 2212 상들의 피크들의 비율은 증가되었고, 시편 내 2223 상의 비율은 감소하고 2212상의 비율은 증가되었다.다.은 증가되었다.다.

• 한국재료학회지
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• 제7권2호
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• pp.157-161
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• 1997

$Bi_{2}Sr_{2}Ca_{0.8}Y_{0.2}Cu_{2}^{16}O_{8+\delta}$의 $^{16}O$이 $^{18}O$으로 치환되는 $^{16}O-^{18}O$ 교환반응의 결정학적 위치 의존성에 대하여 고찰하였다. $Bi_{2}Sr_{2}Ca_{0.8}Y_{0.2}Cu_{2}^{16}O_{8+\delta}$의 라만스펙트럼 측정결과 297, 464, $623cm^{-1}$에서 라만밴드가 관찰되었으며 이들은 모두 시료중의 $^{16}O$이 $^{18}O$으로 치환됨에 따라 저파수측으로 이동하였다. 이러한 동위체 치환에 따른 저파수측으로의 이동속도는 297, $464cm^{-1}$ 라만밴드의 경우 거의 같았지만 $623cm^{-1}$ 라만밴드의 경우 두 라만밴드보다 현저히 늦었다. 이는 $^{16}O-^{18}O$ 교환반응이 산소의 결정학적 위치에 의존한다는 사실을 시사한다. 이로부터 정방정계를 가정하고 623, 464, $297cm^{-1}$ 라만밴드를 각각 $O_{pl}(A_{g}),\;O_{ap}O_{Bi}$의 모드로 귀속하였다.

• 한국세라믹학회지
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• 제38권12호
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• pp.1104-1109
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• 2001

110K상의 산화물 고온초전도체를 B $i_{1.84}$P $b_{0.34}$S $r_{1.91}$C $a_{2.03}$C $u_{3.06}$ $O_{10+}$$\delta$/의 출발조성비로 고상반응법(solid-state reaction)에 의해 합성하였다. 이렇게 합성된 Bi계 110K상의 산화물 고온초전도 물질을 다시 분말 상태로 만든 후, Ag 금속분말을 10wt%, 30wt%, 50wt%의 각 비율로 혼합하였다. Ag 금속분말이 혼합된 시편들을 86$0^{\circ}C$~875$^{\circ}C$로 24시간 동안 최종 소결시켰다. 그후, 각 시편들에 대하여 x-선, $T_{c}$, SEM 등을 측정하여 Ag 혼합량에 대한 초전도특성 및 표면의 grain 크기변화 등에 대한 조사를 진행하였다. Ag 혼합량이 증가됨에 따라 Ag peak의 강도는 증가되었고, 시편 내 2223 상의 비율은 감소하고 2212상의 비율은 증가되었다.비율은 증가되었다.

• 한국분말야금학회:학술대회논문집
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• 한국분말야금학회 2006년도 Extended Abstracts of 2006 POWDER METALLURGY World Congress Part2
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• pp.1239-1240
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• 2006

Effects of $Ag_2O$ doping on the electromagnetic properties in the BiSrCaCuO superconductors. The electromagnetic properties of $Ag_2O$ doped and undoped BiSrCaCuO superconductor were evaluated to investigate the contribution of the pinning centers to the magnetic effect. It was confirmed experimentally that a large amount of magnetic flux was trapped in the $Ag_2O$ doped sample than that in the undoped one, indicating that the pinning centers of magnetic flux are related closely to the occurrence of the magnetic effect. It is considered that the area where normal conduction takes place increases by adding $Ag_2O$ and the magnetic flux penetrating through the sample increases. The results suggested that Ag acts to increase pinning centers of magnetic flux, contributing to the occurrence of the electromagnetic properties.

• Journal of Electrical Engineering and Technology
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• 제2권1호
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• pp.102-105
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• 2007

Effects of $Ag_2O$ doping on the electromagnetic properties in the BiSrCaCuO superconductors. The electromagnetic properties of the $Ag_2O$ doped and undoped BiSrCaCuO superconductor were evaluated to investigate the contribution of the pinning centers to the magnetic effect. It was confirmed experimentally that a large amount of magnetic flux was trapped in the $Ag_2O$ doped sample than that in the undoped one, indicating that the pinning centers of magnetic flux are related closely to the occurrence of the magnetic effect. It is considered that the area where normal conduction takes place increases by adding $Ag_2O$ and the magnetic flux penetrating through the sample increases. The results suggested that Ag acts to increase the pinning centers of the magnetic flux, contributing to the occurrence of the electromagnetic properties.

• Progress in Superconductivity
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• 제5권1호
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• pp.5-8
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• 2003

We studied the effect of spin injection on tunneling conduction properties of intrinsic Josephson junctions formed in $Bi_2$$Sr_2$$CaCu_2$$O_{ 8＋x}$ single crystals. properties of an identical stack (10${\times}$5.0${\times}$0.030 $\mu\textrm{m}^3$) of intrinsic Josephson junctions were compared for the bias current injected through Au and Co electrodes. The suppression of the superconducting gap in the $_2$ double layers and the interlayer Josephson critical current was manifested in the tunneling current-voltage characteristics of the stacks. This effect appears to be caused by the pair breaking associated with spin-polarized carriers injected from the Co electrode into the $Bi_2$$Sr_2$$_2$O$CaCu_{ 8＋x}$ single crystal. This study may provide valuable information on clarifying the mechanism of high- $T_{c}$ superconductivity.y.y.

• Bulletin of the Korean Chemical Society
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• 제11권1호
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• pp.25-28
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• 1990

The superconducting properties have been studied for high-Tc superconductors of the $Bi_{2-x}Mo_xSr_2Ca_2Cu_3O_y$ system (x = 0.03-0.30). The crystal structure is pseudo tetragonal with the average lattice parameters a = 5.38 ${\AA}$, b = 5.44 ${\AA}$ and c = 30.6 ${\AA}$. All samples exhibit superconductivity with Tc offset at 79 K and Tc onset at 90-115 K. The Tc onset point decreases with increasing x, but the Tc offset points are nearly the same for all samples. Scanning electron micrographs show a special growth behavior of the grains with a plate shape. It is suggested that the decrease in Tc onset points with substitution of Mo for Bi is due to the decrease in lattice parameters and to the p-orbital of Mo. It is concluded that Mo does not play a crucial role in the superconducting transition of the $Bi_2Sr_2Ca_2Cu_3O_y$ system.

• Progress in Superconductivity
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• 제6권1호
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• pp.41-45
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• 2004

Polycrystalline Tl-1223 superconductors with a chemical composition of (Tl, Pb, Bi)TEX>$ (Sr, Ba)<_2$$Ca_2$$Cu_3$$O_{x}$ were synthesized by the solid state reaction method. The optimum chemical composition was $Tl_{0.8}$ $Pb_{0.2}$ $Bi_{0.2}$ $Sr_{1.8}$ $Ba_{0.2}$ $Ca_{2.2}$ $Cu_3$$O_{x}$ And the optimum sintering temperature and time were $905^{\circ}C$ and 7.5h, respectively. The sample was evaluated for their superconducting properties by magnetization measurement. The critical temperature $T_{c}$ is 120 K and the critical current density $J_{c}$ (T=5K, 0T) is estimated to be ∼ $10^{5}$ A/$\textrm{cm}^2$ for $Tl_{0.8}$ $Pb_{0.2}$ $Bi_{0.2}$ $Sr_{1.8}$ $Ba_{0.2}$ $Ca_{2.2}$$Cu_3$$O_{x}$ .

• Progress in Superconductivity
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• 제1권1호
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• pp.1-8
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• 1999

The magnetization and/or resistivity of high $T_c$ superconductors ($YBa_2Cu_3O_{7-\delta}$(YBCO) single crystal, $Bi_2Sr_2CaCu_2O_8$ (Bi-2212) single crystal, $Tl_2Ba_2CaCu_2O_8$ (Tl-2212) film, $HgBa_2Ca_2Cu_3O_8$ (Hg-1223) film) have been measured as a function of magnetic field H and temperature T. The extracted fluctuation part of the magnetization and conductivity exhibits a critical behavior consistent with the three-dimensional XY model. The dynamic critical exponent z does not sensitively vary with a type of the superconductors. The value of z ranges from 1.5 to $1.8{\pm}0.1$. However, the static critical exponent ${\nu}$ is the most largely increased in Tl-2212 that has a weaker interlayer coupling strength than YBCO; the value of ${\nu}$ is 0.669, 0.909, 1.19, and 1.338 for YBCO, Bi-2212, Hg-1223, and Tl-2212 respectively. The results indicate that the weak interlayer coupling along the c-axis of high $T_c$ superconductors near $T_c$ does not influence the dynamic critical exponent z (the same value of superfluid $^4He$), but significantly increases the static critical exponent ${\nu}$.