• 한국전기전자재료학회논문지
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• 제11권6호
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• pp.493-501
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• 1998

$YBa_2Cu_3O_X$ samples were fabricated by MPMG(Melt Powdered Melt Growth). Intitial composition of the mixed powders were prepared as follow ; $YBa_2Cu_3O_X$ : $Y_2BaCuO_5$ = 1:0, 1:0.2, 1:0.3, 1:0.4. After the first melt and cooling, 5wt% to 20wt% fo Ag power was added to the powder. Effects of the different initial $Y_2BaCuO_5$ and Ag addition amount on $J_c$ and magnetization of $YBa_2Cu_3O_X$ fabricated by MPMG method were investigated. The critical current density increased with the amount of $Y_2BaCuO_5$ and Ag. It was also observed that the difference between negative and positive magnetization in the magnetization hysteresis measurement at 77K was larger than the case where $Y_2BaCuO_5$and Ag were not added to the $YBa_2Cu_3O_X$ powders. It is concluded that $Y_2BaCuO_5$ sample with 40wt% amount of $Y_2BaCuO_5$ and 20wt% amount of Ag has not only the largest $J_c$ but also the improved pinning effect.

• Progress in Superconductivity
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• 제13권1호
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• pp.12-17
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• 2011

We investigated the effects of Ba and Cu co-substitution on the structural and superconducting properties of ($Ru_{1-y}Cu_y$)($Sr_{1.67-x}Ba_xEu_{0.33}$)($Eu_{1.34}Ce_{0.66}$)$Cu_2O_z$ samples. X-ray diffraction(XRD) reveals that single-phase samples can be obtained in the range from x = 0.1 to 0.2 for ($Ru_{0.5}Cu_{0.5}$)($Sr_{1.67-x}Ba_xEu_{0.33}$)($Eu_{1.34}Ce_{0.66}$)$Cu_2O_z$ and from y = 0.25 to 0.5 for ($Ru_{1-y}Cu_y$)($Sr_{1.47}Ba_{0.2}Eu_{0.33}$)($Eu_{1.34}Ce_{0.66}$)$Cu_2O_z$, respectively. All samples with compositions of ($Ru_{0.5}Cu_{0.5}$)($Sr_{1.67-x}Ba_xEu_{0.33}$) ($Eu_{1.34}Ce_{0.66}$)$Cu_2O_z$ (x = 0 - 0.33) show superconducting transition behavior and the onset transition temperature decreases slightly with increasing x in consistent with the change of hole concentration estimated from room temperature thermoelectric power measurements. The XRD and resistivity measurements for the ($Ru_{1-y}Cu_y$)($Sr_{1.47}Ba_{0.2}Eu_{0.33}$)($Eu_{1.34}Ce_{0.66}$) $Cu_2O_z$ system indicate that the partial substitution of Cu for Ru is necessary to form phase pure samples, but result in a small change in transition temperature in the single-phase region from x = 0.25 to 0.5.

• 한국세라믹학회지
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• 제32권1호
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• pp.83-89
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• 1995

YBa2Cu3O7-$\delta$, Y2BaCuO5, and binary compounds in the Ba-Cu-O system with the nominal composition of Ba2CuO3, BaCuO2, Ba3Cu4O7, Ba3Cu5O8 were synthesized to investigate the heat evolutions and crystalline phases in the hydration reaction of orthorhombic YBa2Cu3O7-$\delta$ phase. The observed crystalline phases were YBa2Cu3O7-$\delta$, Y2BaCuO5, and BaCuO2, or Ba2Cu3O5＋x, and some amount of noncrystalline phase in the Ba-Cu system comounds. In contact with distilled water, YBa2Cu3O7-$\delta$ and Y2BaCuO5 did not have considerable heat liberation, but in the binary compounds of the Ba-Cu-O system, the amount of total heat liberation was increased with respect to the Cu content. It might be that the reaction of high temperature superconductor YBa2Cu3O7-$\delta$ with water and/or moisture originated from the unusual oxidation state of Cu ion and the presence of amorphous Ba-Cu oxide compound. The degradation of high Tc superconductor by moisture and water could be controlled by restricting the heterogeneous distribution of Tc comlposition and the formation of second phase, such as stable Y2BaCuO5, and the resulting unstable Ba-Cu oxide compound.

• 한국재료학회지
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• 제4권8호
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• pp.870-876
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• 1994

$Y_{1}Ba_{2}Cu_{3}O_{7-\delta}$계에서 211상의 성장거동을 관찰하기 위하여 123시편을 $1100^{\circ}C$에서 유지시간을 변화시켜 MgO다결정 기판과 MgO 단결정 기판위에 놓고 소결시킨 후 공냉하였다. 211입자는 유지 시간이 증가함에 따라 성장하였으며MgO단결정 기판보다 MgO다결정 기판을 사용했을때 더 큰 성장을 보였다. CuO양을 변화시키면서 만든 $Y_{2}Ba_{1+X}Cu_{3}O_{5+\delta}$ 시편에서 211입자는 CuO양이 증가함에 따라 조대해졌으며 0.6mol CuO가 더 첨가된 시편에서 가장 큰 211입자가 관찰되었다. $Y_{2}Ba_{1+X}Cu_{3}O_{5+\delta}$시편에서 211입자는 아주 미세하고 균일하게 분포되었다. $SnO_{2}$첨가로 인한 211입자의 성장억제 효과는 ($BaCuO_{2}$+ CuO)액상에서보다 CuO액상에서 더 크게 나타났다.

• 한국전기전자재료학회논문지
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• 제28권2호
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• pp.80-84
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• 2015

We investigated the dielectric relaxation properties $0.5Ba(Zr_{0.2}Ti_{0.8})O_3-0.5(Ba_{0.7}Ca_{0.3})TiO_3$ ceramics with CuO addition. With increasing CuO addition, the lattice parameter was increased by substitution of small amount $Cu^{2+}$ ion in B-site of $0.5Ba(Zr_{0.2}Ti_{0.8})O_3-0.5(Ba_{0.7}Ca_{0.3})TiO_3$ ceramics. Also the grain size and the maximum dielectric constant of $0.5Ba(Zr_{0.2}Ti_{0.8})O_3-0.5(Ba_{0.7}Ca_{0.3})TiO_3$ ceramics was decreased with increasing amounts of CuO addition. Moreover, the diffused phase transition properties (${\gamma}$) of $0.5Ba(Zr_{0.2}Ti_{0.8})O_3-0.5(Ba_{0.7}Ca_{0.3})TiO_3$ ceramics was increased by compositional fluctuation with increasing of CuO amount, changed from 1.45 at 1 wt% CuO addition to 1.94 at 7 wt% CuO addition.

• 공업화학
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• 제10권5호
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• pp.772-777
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• 1999

$Y_2Ba_1Cu_1O_5(Y211)$ 분말은 출발물질로서 $Y_2O_3(99.9%)$, $BaCO_3(99.9%)$, and CuO(99.9%) 분말을 사용하여 고상반응법과 발화합성법을 이용하여 제조하였다. $Y_2Ba_1Cu_1O_5(Y211)$ 분말에 대한 상형성과 반응속도는 열처리 온도와 반응시간에 따른 시료들을 X-선 회절분석을 이용하여 연구하였다. X-선 회절선으로부터 측정된 전화율($X_{211}$)과 반응특성으로부터 상 형성속도가 분말의 입자크기에 의해 지배되는 것을 알 수 있었다. 그리고 발화합성법으로 제조된 Y211상의 활성화에너지(${\Delta}E_a$)는 고상반응법에 의해 제조된 것의 149.46 kJ/mol과 비교할 때 136.42 kJ/mol을 나타내었다. $Y_2Ba_1Cu_1O_5$계에서의 활성화에너지 값은 발화합성법이 고상반응법보다 더욱 효율적인 방법임을 보였다.

• 한국결정성장학회지
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• 제4권2호
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• pp.148-156
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• 1994

$YBa_2Cu_3O_X$상 부근의 3가지 조성을 skull melting 방법으로 4MHz에서 녹인 후 방향적 결정성장을 시켰다. 일반적인 무기재료 공정방법으로 처리된 분말을 skull에 넣은 후 $1200^{\circ}C$부근에서 용융시켰다. 사용한 성장속도는 4~0.25 cm/hr이었으며, 금속현미경, X-선 회절기, EDX 등을 이용해서 제조된 시편을 조사하여 사용한 분말의 조성에 따른 시편의 미세조직의 변화를 관찰하였다. $YBa_2Cu_7O_X$와 $YBa_5Cu_{11}O_X$ 시편의 대표적인 미세조직은 성장방향으로 자라난 침상형태의 $YBa_2Cu_3O_X$와 $Y_2BaCuO_5$ 상이 $CuO-BaCuO_2$의 공융 조직상 사이에 생성된 것으로 나타났다.

• Transactions on Electrical and Electronic Materials
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• 제5권2호
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• pp.81-85
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• 2004

High T$\_$c/ (Sm/Y)$\_$1.8/Ba$\_$2.4/Cu$\_$3.4/O$\_$7-$\delta$/ ［(Sm/Y)］ superconductor, a combination of Y and Sm(50% each), was systematically investigated by the zone melt growth process. A sample prepared by this method showed well-textured microstructure, and (Sm/Y)$_2$BaCuO$\_$5/［(Sm/Y)211］inclusions were uniformly dispersed in large (Sm/Y)Ba$_2$Cu$_3$O$\_$y/ ［(Sm/Y)123］matrix. The sample showed a sharp superconducting transition at 91 K. The magnetization measurements of the (Sm/Y)1.8 sample exhibited the enhanced flux pinning, compared with Y$\_$1.8/Ba$\_$2.4/Cu$\_$3.4/O$\_$7-$\delta$/(Y1.8) sample without Sm. Critical current densities of (Sm/Y) 1.8 sample was 3.5${\times}$10$^4$A/$\textrm{cm}^2$ at 1 T and 77 K.

• Bulletin of the Korean Chemical Society
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• 제10권1호
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• pp.5-8
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• 1989

Conventional ceramic method has been used to prepare the green phase, $Y_2BaCuO_5$, commonly observed in 90-K superconductor $YBa_2Cu_3O_P{7-{\delta}}$as an impurity phase. The powder X-ray diffraction analysis indicates that $Y_2BaCuO_5$ has an orthorhombic symmetry with lattice parameter of a = 12.2 $\AA$, b = 5.61 $\AA$, and c = 7.14 $\AA.$ The average g-value 2.13 observed in ESR spectrum is attributable to Cu2+ stabilized in $C_{4v}$ field. From the magnetic susceptibility ($\mu$eff = 2.29 BM) and the ESR measurements, it is confirmed that Cu(II) $3d^9$ electrons in $Y_2BaCuO_5$ are localized and can be characterized by Curie-Weiss behavior. Optical reflectance spectrum shows a broad absorption peak around 680 nm due to dxy ${\rightarrow}$ $dx^2-y^2$ eletronic transition.

• 한국재료학회지
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• 제5권7호
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• pp.786-793
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• 1995

Ag를 $Y_1$Ba$_2$Cu$_3$O$_{7-y}$에 첨가하여 고상반응법으로 시료를 제작, Ag가 $Y_1$Ba$_2$Cu$_3$O$_{7-y}$의 고온초전도성과 그의 미세구조에 미치는 영향을 조사하였고 그에 따른 기계적 특성을 연구하였다. Ag의양이 증가함에 따라 결정립의 크기가 증가하였고 연결성이 향상되어 시료의 결정구조가 치밀해지고 단단해졌으며 결정립간의 weak link와 weak coupling을 줄이고 균일한 초전도 상을 형성시킨다는 것을 알 수 있었다. 또한 $Y_1$Ba$_2$Cu$_3$O$_{7-y}$결정구조의 이방성을 줄였고 $Y_1$Ba$_2$Cu$_3$O$_{7-y}$의 열적 안정성을 향상 시켰음을 알 수 있었다. 그리고 Ag의 첨가에 따라 시료의 기계적 강도가 증가함을 보였다.가함을 보였다.