• Title/Summary/Keyword: BiPbSrCaCuO system

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A Study on the Characteristic of High Tc Oxide Superconductor, Bi-Pb-Sr-Ca-Cu-O System (Bi-Pb-Sr-Ca-Cu-O계 산화물 고온초전도체의 특성에 관한 연구)

  • Kim, Y.S.;Lee, M.S.;Lee, M.S.;Jin, Y.C.
    • Journal of the Korean Society for Heat Treatment
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    • v.4 no.1
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    • pp.13-18
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    • 1991
  • The formation of high $T_c$ phase is very sluggish and c parameter of unit cell of high $T_c$ phase is about $37{\AA}$. High $T_c$ oxide superconductor with a $T_c$ above 100 K has been successfully prepared by solid state reaction method in BiSrCaCuO system by Pb adding. The microstructure related to the formation of the high $T_c$ phase has been investigated. As compared with YBCO compound, the formation reaction of the high $T_c$ requires long time heat treatment. It is due to the transformation from the low $T_c$ phase to high $T_c$ phase. The sintering just below the melting point of the calcined powder mixture is effective on the formation of the high $T_c$ phase in Pb-added BiSrCaCuO system. The growth of the high $T_c$ superconducting phase has a thin plate shape, which is characterized by the c parameter of $37{\AA}$. The formation of the high $T_c$ phases is delayed by the excessive addition of Pb. The lattice parameter(c) of the unit cell (both the low and high $T_c$ phases) is increased with increase of Pb.

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Effects of Sb-Incorporation on the 2223 Phase in the Superconducting Bi-Pb-Sr-Ca-Cu-O System

  • Seong Han Kim;Dong Hoon Lee;Jong Sik Park;Seung Koo Cho;Sung Han Lee;Keu Hong Kim
    • Bulletin of the Korean Chemical Society
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    • v.15 no.2
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    • pp.115-118
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    • 1994
  • Samples of ($Bi_{2-x}Sb_x)PbSr_2Ca_2Cu_3O_y$, compositions with x=0.0, 0.1, and 0.2 were prepared by solid-state reaction. The solubility of Sb into the 2223 phase is lower than 0.05 for the ratio of Sb/Bi. The lack of stability of the Sb-substituted $Bi_2O_2$ double layers is likely to cause the solubility low. There is no great dependence of lattice parameters on the Sb-content, and bonds around the square-pyramidal Cu atom are not affected by the $Sb^{3+}$ ion substituted. The superconducting transition temperature of this system is decreased gradually with increase of Sb, which is tentatively attributable to the perturbation of the Bi 6p-O 2p band and/or to the low volume fraction of the 2223 phase.

Magnetic Properties of BiPbSrCaCuO System (Bi계 초전도체의 자기적 효과)

  • 이상헌
    • Proceedings of the Korea Institute of Applied Superconductivity and Cryogenics Conference
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    • 2002.02a
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    • pp.355-357
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    • 2002
  • The relationship between magnetic properties of BiPbSrCaCuO superconductor and externally applied magnetic field was studied to develop a magnetic field polarity sensor. The behavior was related to the magnetic flux trapped in the superconductor, which penetrates through the material by the external magnetic field. Some portion of the superconductor was changed to a normal state by the trapped magnetic flux. Electrical characteristics of the superconductor with trapped magnetic flux were extremely sensitive to the external magnetic field and showed different responses depending on the direction of the magnetic field.

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Direct Preparation of fine Powders of Bi-Pb-Sr-Ca-Cu-O by Ultrasonic Spray Pyrolysis (초음파 분무열분해에 의한 Bi-Pb-Sr-Ca-Cu-O의 미분체 제조)

  • 주명희;박도순;김윤수
    • Journal of the Korean Ceramic Society
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    • v.28 no.5
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    • pp.353-358
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    • 1991
  • Fine powders of the 2212 superconducting phase of bismuth system have been prepared directly from solution using ultrasonic spray pyrolysis. The fine superconducting powders produced by pyrolysis were characterized for the size, shape, and crystalline phase by SEM and XRD. The pyrolysis temperature, flow rate of the carrier gas, residence time of the droplets greatly influenced the size, shape, and crystalline phase. The optimum temperature and flow rate of the carrier gas for the preparation of fine powders of the 2212 superconduting phase were found to be 830$^{\circ}C$and 3ι/min, respectively.

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Formation of the precipitates in the Bi-2223/Ag superconducting tapes by post-heat treatment (Bi-2223 초전도 선재의 후열처리 과정에 의한 석출물의 형성)

  • Lee, Sang-Hee;Kim, Cheol-Jin;Chung, Jun-Ki;Yoo, Jae-Moo;Ko, Jae-Woong
    • 한국초전도학회:학술대회논문집
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    • v.10
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    • pp.262-267
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    • 2000
  • To tap the possibility of exploiting the precipitates as flux-pinning center in the Bi-2223 superconducting system, as-received Bi-2223/Ag tapes with the starting composition of Bi$_{1.8}$Pb$_{0.4}$Sr$_2$Ca$_{2.2}$Cu$_3$O$_8$ were post-annealed at various temperature, oxygen partial pressure, and annealing time. The 2$^{nd}$ phases in the annealed specimen were analysed with XRD, SEM, TEM, and EDS. The size and the distribution of the precipitates such as (Ca,Sr)$_2$(Pb,Bi)O$_4$ and Bi$_{0.5}$Pb$_3$Sr$_2$Ca$_2$CuO$_{12+{\delta}}$ (3221) in the Bi-2223 matrix was controllable by varying heat-treatment condition without breaking the connectivity of the 2223 grains. The nano-size precipitates within the 2223 grains are conjectured as working as flux-pinning sites, resulting in increased J$_c$ value.

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The Precipitation of Second Phases by Annealing Heat Treatment in the $(Bi,Pb)_2$${Sr_2}{Ca_2}{Cu_3}{O_{10}}$ Superconductor System (BSCCO계 초전도체에서 서냉 열처리에 의한 2차상 석출)

  • 이상희;김철진;유재무
    • Journal of the Korean Ceramic Society
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    • v.37 no.12
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    • pp.1212-1220
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    • 2000
  • Bi-2223 초전도체계에서 석출물을 flux-pinning center로 이용할 수 있는지 가능성을 타진하기 위하여 $Bi_{1.8}$P $b_{0.4}$S $r_{2}$C $a_{2.2}$C $u_3$ $O_{8}$ 조성을 가진 Bi-2223/Ag 선재를 반응온도, 산소분압, 시간 등을 변화시키면서 열처리를 행하였다. 열처리 후 석출물들은 XRD, SEM, TEM, EDS로 분석하였다. Bi-2223 모상내의 (Ca, Sr)$_2$(Pb,Bi) $O_4$, B $i_{0.5}$ P $b_3$S $r_2$C $a_2$Cu $O_{12+}$$\delta$/ (3221)와 같은 2차상들의 크기와 분포는 2223 입자들의 연결성을 파괴하지 않고 열처리 조건에 의해서 조절할 수 있었다. 서냉 열처리가 된 시편은 임계전류밀도( $J_{c}$)값이 증가하였는데, 이는 2223 입자내 나노미터 크기로 형성된 석출물들이 flux-pinning sites로 작용한 것으로 추정된다.다.

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The Effect of Sintering Time on the Stabilization of the Bi-Pb-Sr-Ca-Cu-O Superconducting Phase (Bi-Pb-Sr-Ca-Cu-O 초전도상의 안정화에 미치는 소결시간의 영향)

  • 형경우;박성호;이두원;한태종;최범식;김창은
    • Journal of the Korean Ceramic Society
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    • v.29 no.2
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    • pp.95-100
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    • 1992
  • A high-Tc superconducting phase was obtained using long sintering time of 210 hours. From XRD and SEM analyses, it could be confirmed that the particles were plate phase, of which the structure is tetragonal system with lattice parameter a=b=5.44${\AA}$, C=37.18${\AA}$. Resistance and current density measurements were carried out using 4 probe method. The experimental data revealed that the stable high-Tc superconducting phase was easily formed by addition of Pb to Bi-system. Therefore, we could find the sintering condition to synthesis the system having the largest fraction of high Tc phase.

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Effect of La0.7Sr0.3MnO3 addition on superconducting properties and local structure of (Bi, Pb)-2223 superconductor

  • M. A. Anugrah;R. P. Putra;J. Y. Oh;B. Kang
    • Progress in Superconductivity and Cryogenics
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    • v.25 no.2
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    • pp.5-9
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    • 2023
  • The effect of La0.7Sr0.3MnO3 (LSMO) addition on the superconducting property of Bi1.6Pb0.4Sr2Ca2Cu3O10+δ ((Bi, Pb)-2223) polycrystalline samples was studied. LSMO (0.3 wt.% to 2.0 wt.%) added (Bi, Pb)-2223 samples were prepared by using a solid-state reaction method. The XRD analyses show that as the LSMO addition increases, the volume fraction of the Bi-2223 phase is gradually decreased. The critical temperature (Tc) exhibits a gradual decrease with a single transition as the LSMO amount increases up to 1.0 wt.%, but a further addition of LSMO induces an abrupt decrease of Tc with a dual transition. The analyses on the local structure of the CuO2 plane from the X-ray absorption fine structure (EXAFS) measurements showed that for the samples with low concentration of LSMO up to 1.0 wt.%, the Cu-O bond length and the CuO2 plane ordering do not degrade from the values of pure (Bi, Pb)-2223, while they get worsen with a further increase of LSMO addition. These results open up the possibility of LSMO as artificial pinning centers of the (Bi, Pb)-2223 system for power application.

Effect of Mechanical Grinding on the superconducting Characteristics in the Bi(Pb)SrCaCuO System (Grinding 조건이 Bi(Pb)SrCaCuO 계(系) 초전도체의 상변이에 미치는 영향)

  • Cho, H.D.;Jang, K.W.;Park, Y.P.;Lee, J.U.
    • Proceedings of the KIEE Conference
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    • 1991.07a
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    • pp.201-203
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    • 1991
  • T. Kanal et al, were studied the superconducting properties in Bi system by mechanical grinding, in which the authors found that the samples ground degraded from the superconducting phases to nonsuperconducting phases. To obtain more information of the practical application in Bi system with high-Tc phase in this paper, these samples mechanically ground and the high-Tc phase properties of grinding powder samples were investigated.

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The Powder Synthesis of (Bi,Pb)-2223 System Superconductor by Oxalate Method and Thick Film Preparation (옥살산염법에 의한 (Bi, Pb)-2223계 초전도 분말 합성과 후막 제조)

  • 하성원;김형태;이응상
    • Journal of the Korean Ceramic Society
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    • v.34 no.10
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    • pp.1083-1091
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    • 1997
  • As one of the chemical powder fabrication methods, the powder preparation method by using oxalate has the following advantages; (1) easy to control the chemical stoichiometry, (2) easy to fabricate homogeneous and fine particles, and (3) easy to be thermaly decomposed at low temperature. In the present study, the initial morphology and size distribution of the powder were controlled and the homogeniaty was improved. By carefully controlling the pH with NH4OH, the Bi(Pb)-Sr-Ca-Cu-O superconducting powders were prepared and investigated for their properties. The microstructures and the superconducting properties of the pelletized samples were investigated. Also, the microstructures and electrical properties of the samples prepared by tape casting method were investigated. The fabricated powders were spherical with less than 400 nm, but most of them were agglomerated to be 1~3 ${\mu}{\textrm}{m}$ in size. The critical temperature of the pelletized sample annealed at 84$0^{\circ}C$ for 72 hours in air was 110K. And the critical currents of annealed samples in air prepared by tape casting process for 24 hours and 72 hours were 0.6 A (Jc=600A/$\textrm{cm}^2$) and 1.9A (Jc=1, 900A/$\textrm{cm}^2$) respectively.

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