• Applied Chemistry for Engineering
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• v.9 no.2
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• pp.165-171
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• 1998

The $Y_1Ba_2Cu_3O_{7-x}$(123) superconductor powders were prepared by pyrophoric synthesis method(PSM) using $Y_2O_3$(99.9%), $BaCO_3$(99.9%), and CuO(99.9%) powders. The phase formation and reaction kinetics of 123 superconductor manufactured with powders prepared in various pHs of pyrophoric synthetic solution have been studied through the experiments at various heat treatment temperatures and times. Inductively coupled plasma(ICP) spectroscopy and scanning electron microscopy(SEM) measurements were performed to examine the composition and morphology of the sample. X-ray diffraction(XRD) analysis was done to determine phase formation and conversion ratio of Y-Ba-Cu-O systems. The 123 powder prepared at pH 7(${\pm}0.3$) yields the best result in terms of purity, homogeneity, and reactivity. The activation energies(${\Delta}E_a$) of 123 phase formation were found to be 191 kJ/mol and 230kJ/mol in solid state reaction method and pyrophoric synthesis method, respectively.

• Proceedings of the Materials Research Society of Korea Conference
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• 1997.05a
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• pp.46-46
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• 1997

• Progress in Superconductivity and Cryogenics
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• v.18 no.4
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• pp.1-4
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• 2016

We investigated the relation between the Cu-O bond length and the superconducting properties of $BaSnO_3$ (BSO)-added $GdBa_2Cu_3O_{7-x}$ (GdBCO) thin films by using extended x-ray absorption fine structure (EXAFS) spectroscopy. 4 wt.% $BaSnO_3$ (BSO) added $GdBa_2Cu_3O_{7-x}$ (GdBCO) thin films with varying thickness from $0.2{\mu}m$ to $1.0{\mu}m$ were fabricated by using pulsed laser deposition (PLD) method. The transition temperature ($T_c$) and the residual resistance ratio (RRR) of the GdBCO films increased with increasing thickness up to $0.8{\mu}m$, where the crystalline BSO has the highest peak intensity, and then decreased. This uncommon behaviors of $T_c$ and RRR are likely to be created by the addition of BSO, which may change the ordering of GdBCO atomic bonds. Analysis from the Cu K-edge EXAFS spectroscopy showed an interesting thickness dependence of ordering behavior of BSO-added GdBCO films. It is noticeable that the ordering of Cu-O bond and the transition temperature are found to show opposite behaviors in the thickness dependence. Based on these results, the growth of BSO seemingly have evident effect on the alteration of the local structure of GdBCO film.

• Korean Journal of Materials Research
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• v.2 no.3
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• pp.197-201
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• 1992

The temperature dependence of the magentic moment was determined for the system of high $T_{c}$ superconductor $Y_{1-X}Sm_{x}Ba_2Cu_3O_{7-y}$ with x=0, 0.2, 0.4, 0, 6, 0.8 and 1.0. Also the magnetic susceptibility and the magnetic critical current density were measured from the magnetic hysterisis loops obtained at 30 K. From the results of the magnetic susceptibility measurements, the high $T_{c}$ phase were ranged from 14.7 to 49.1%. The values of the magnetic critical current densities were in the range of $10^3~10^4A/cm^2$. The penetration depth was approximately ninety times larger than the coherence length.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.16 no.4
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• pp.336-342
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• 2003

(Sm/Y)$_{1.8}$B $a_{2.4}$C $u_{3.4}$$O_{7-x}$ [(Sm/Y)1.8] high $T_{c}$ superconductors were directionally grown by Rod-type Seed Melt Growth(RSMG) process in air atmosphere. The sintered polycrystalline N $d_{1.8}$B $a_{2.4}$C $u_{3.4}$$O_{7-x}$(Nd1.8) of rod-type seed crystal grown by extrusion mold process were used for achieving the ab-plane alignment haying large grains perpendicular to the center of (Sm/Y)1.8 samples. The observations using TEM micrographs of the melt-textured (Sm/Y)1.8 samples revealed that the nonsuperconducting (Sm/Y)211 inclusions are uniformly distributed in the superconducting (Sm/Y)123 matrix. The microstructure and superconducting properties were investigated by XRD, TEM and SQUID magnetometer. The RSMG (Sm/Y)1.8 samples showed an onset $T_{c}$ $\geq$ 90 K and sharp superconducting transition.nsition.ion.nsition.

• Journal of the Korean Institute of Telematics and Electronics
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• v.27 no.5
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• pp.724-728
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• 1990

The X-ray diffraction pattern, electrical resistance, density and critical temperature of a series of YBa2(Cu3-xNix)O7-\ulcornersamples (0\ulcorner\ulcorner.5) were investigated with the increase of the Ni content. The samples show a principal 1.2.3-like phase with well resolved orthorhombic peaks. The final pattern of the x=0.1 sample appears to be well reacted orthorhombic YBa2(Cu,Ni)3O7-\ulcornerwith minor impurities and an appreciable amorphous fraction. From the above results, we conclude that Ni does not play an important role for the superconductivity in the Y-Ba-Cu-O system.

• Electrical & Electronic Materials
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• v.4 no.4
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• pp.330-337
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• 1991

y의 크기가 0.02에서부터 2.0까지의 두 차수만큼 변하게 불소가 첨가된 YBa$_{2}$Cu$_{3}$$O_{7-x}$F$_{y}$ 초전도물질을 금속질산염과 수산화나트륨 및 불화나트륨을 써서 졸-겔법으로 제조하였다. 불소함유양들을 이온-선택 전극을 사용하여 측정하였다. 반응물질로 첨가된 불소전부가 최종시료속에 존재한다는 것을 알았다. XRD 관측으로부터 y.leq.0.2인 시료들은 단지 단상 페로브스카이트 구조로 되었고 반면 y.geq.0.5인 것들은 최종시료속에 BaF$_{2}$ YF$_{3}$및 CuO와 같은 화합물들과 함께 생성되어져 있다고 결론지을 수가 있다. 더구나 고체 $^{19}$ F 핵자기공명관측이 불소가 정말로 격자위치들 속에 혼입되어 있는지 여부를 확인하기 위하여 행해졌는데 실험결과로부터 YBa$_{2}$Cu$_{3}$$O_{7-x}$ 격자위치속에 혼입된 불소의 몰비는 화합물 1몰당 약 0.2라는 것을 보여주었다. 또한 전기저항률의 측정은 개시감계온도가 y.leq.0.2와 같이, 지정된 첨가율이 적은 영역에서는 y의 증가에 따라 약간씩 증가하는 경향이 있음을 보여주고 있다.

• Progress in Superconductivity
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• v.6 no.1
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• pp.13-18
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• 2004

High-.ate in-situ$ YBa_2$Cu$Cu_3$$O_{7-x}$ (YBCO) film growth was demonstrated by means of the electron beam co-evaporation. Even though our oxygen pressure is low, ∼$5 ${\times}$10^{-5}$ Torr, we can synthesize as-grown superconducting YBCO films at a deposition rate of around 10 nm/s. Relatively high temperatures of around 90$0^{\circ}C$ was necessary in this process so far, and it suggests that this temperature at a given oxygen activity allows a Ba-Cu-O liquid formation along with an YBCO epitaxy. Local critical current density shows a clear correlation with local resistivity. Homogeneous transport properties with a large critical current density ($4 ∼ 5 MA/\textrm{cm}^2$ at 77K, 0T) are observed in top faulted region while it is found that the bottom part carries little supercurrent with a large local resistivity. Therefore, it is possible that thickness dependence of critical current density is closely related with a topological variation of good superconducting paths and/or grains in the film bodies. The information derived from it may be useful in the characterization and optimization of superconducting films for electrical power and other applications.

• Journal of the Korean Ceramic Society
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• v.27 no.1
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• pp.43-47
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• 1990

An attempt was made to grow Y-Ba-Cu-O single crystals by skull method(cold crucible process). Grown YBa2Cu3O7-x(YBC) single crystals were obtained from the upper part of the YBC solid mixture. There were plate-like YBC single crystals aligned with solidified flux along the crystal growth direction. Single crystal size was (5$\times$2$\times$0.2㎣) and was grown to a-b plane of YBC crystal structure which can flow super currents. Optical microscope and X-ray diffraction were employed characterize these microstructure and YBC single crystals.

• Journal of the Korean Chemical Society
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• v.37 no.7
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• pp.683-686
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• 1993