• Title/Summary/Keyword: High $T_c$ superconductor

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Effect of the Ag Additive on the ${Bi_{1.84}}{Pb_{0.34}}{Sr_{1.91}}{Ca_{2.03}}{Cu_{3.06}}{O_{10+\delta}}$(110K Phase) High-$T_{c}$ Susperconductor (${Bi_{1.84}}{Pb_{0.34}}{Sr_{1.91}}{Ca_{2.03}}{Cu_{3.06}}{O_{10+\delta}}$(110K 상) 산화물 고온초전도체에 미치는 Ag 혼합효과)

  • 이민수;최봉수;최봉수
    • Journal of the Korean Ceramic Society
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    • v.38 no.12
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    • pp.1104-1109
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    • 2001
  • Samples with the nominal composition, B $i_{1.84}$P $b_{0.34}$S $r_{1.91}$C $a_{2.03}$C $u_{3.06}$ $O_{10+}$$\delta$/ high $T_{c}$ superconductors containing As as an additive were fabricated by a solid-state reaction method. Samples with Ag of 10wt%, 30 wt% and 50 wt% each were sintered at 86$0^{\circ}C$~875$^{\circ}C$ for 24 hours. The structural characteristics, critical temperature and grain size with respect to Ag contents were analyzed by XRD(X-ray Diffraction) and SEM(Scanning Electron Microscope), respectively. As Ag contents increased, XRD peaks of g in Bi-2223 phase superconductors intensified and the proportion of the phase transition from Bi-2223 to Bi-2212 was increased.increased.

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Anisotropic superconductivity of high quality FeSe1-x Single crystal

  • Kwon, Chang Il;Ok, Jong Mok;Kim, Jun Sung
    • Progress in Superconductivity and Cryogenics
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    • v.16 no.4
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    • pp.26-30
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    • 2014
  • We investigate the upper critical field anisotropy ${\Gamma}_H$ and the magnetic penetration depth anisotropy ${\Gamma}_{\lambda}$ of a high-quality $FeSe_{1-x}$ single crystal using angular dependent resistivity and torque magnetometry up to 14 T. High quality single crystals of $FeSe_{1-x}$ were successfully grown using $KCl-AlCl_3$ flux method, which shows a sharp superconducting transition at $T_C{\sim}9K$ and a high residual resistivity ratio of ~ 25. We found that the anisotropy ${\Gamma}_H$ near $T_C$ is a factor of two larger than found in the poor-quality crystals, indicating anisotropic 3D superconductivity of $FeSe_{1-x}$. Similar to the 1111-type Fe pnictides, the anisotropies ${\Gamma}_{\lambda}$ and ${\Gamma}_H$ show distinct temperature dependence; ${\Gamma}_H$ decreases but ${\Gamma}_{\lambda}$ increases with lowering temperature. These behaviors can be attributed to multi-band superconductivity, but different from the case of $MgB_2$. Our findings suggest that the opposite temperature dependence of ${\Gamma}_{\lambda}$ and ${\Gamma}_H$ is the common properties of Fe-based superconductors.

19F NMR Study of Fluorinated YBa2Cu3O7-x

  • Lee, Cheol-Eui;D. White;P. K. Davies;S. J. Noh
    • Journal of Magnetics
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    • v.2 no.2
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    • pp.35-37
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    • 1997
  • A sample of YBa2Cu3O7-x fluorinated by a high temperature (400$^{\circ}C$) gas exchange technique has been investigated by means of 19F NMR (nuclear magneti resonance) measurements in both superconducting and normal state. As a result, behaviors characteristic of the superconductor, including a peculiarity in the spin-lattice relaxation rate (1/T1) around 250 K, were observed.

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Study of Partial Discharge Degradation of Insulating Materials in Liquid Nitrogen (액체$N_2$중 절연재료의 부분방전 열화 연구)

  • Kim, H.H.;Kim, S.H.;Ma, D.Y.;Chang, J.K.;NamGung, D.;Cho, J.W.
    • Proceedings of the KIEE Conference
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    • 1995.11a
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    • pp.406-410
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    • 1995
  • A superconducting cable is one of the promising methods of undground transmission of high electric power in the future. It is very important that composite insulation system of $LN_2$ and polymer films takes into consideration for application high $T_c$ superconductor. This study is about both the partial discharge and properties V-t in $LN_2$. As result, applied voltage doesn't depend on the radius of non-eroded area but eroded area. And eroded area is observed the formation such as the ring of a tree.

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A New Superconductor with the 1212 Structure $(Pb,Sn)Sr_2(Ca,Lu)Cu_2O_z$

  • Lee, Ho-Keun;Jee, Chan-Soo
    • Progress in Superconductivity
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    • v.2 no.1
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    • pp.6-10
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    • 2000
  • New cuprates with the nominal composition $(Pb_{0.75}Sn_{0.25})Sr_2(Ca_{1-x}Lu_x)Cu_2O_z(x=0.4{\sim}1.0)$ have been synthesized. These materials exhibit superconducting properties for 0.4 $\leq$ x $\leq$ 0.7. It is also observed that the superconductivity of the as-prepared sample is enhanced by post-annealing at high temperature followed by quenching. X-ray diffraction analysis reveals that the c lattice parameter decreases as x increases whereas the a lattice parameter is nearly independent of the value of x for both the as-prepared and the post-treated samples. The thermoelectric power measurements indicate that the post-heat-treatments result in an increase in the hole carrier density which account for the observed increase of $T_c$. Bulk superconductivity with a $T_c$ value of 60 K is observed in this system.

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$^{63}Cu$ NQR Study of the Anisotropy in $YBa_{2}Cu_{3}O_{7}$ ($YBa_{2}Cu_{3}O_{7}$의 비등방성에 관한 $^{63}Cu$ 핵사중극공명 연구)

  • B. Chang;Cheol-Eui Lee
    • Journal of the Korean Magnetics Society
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    • v.4 no.1
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    • pp.48-51
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    • 1994
  • We have studied the room temperature anisotropy in the high $T_{c}$ superconductor $YBa_{2}Cu_{3}O_{7}$ by means of the $^{63}Cu$ nuclear quadrupole resonance (NQR). For the magnetically oriented powder samples, NQR signals were obtained only when the RF magnetic field is applied perpendicular to the direction of the crystalline c-axis. Significant differences in the spin-lattice relaxation times ($T_{1}$) and the lineshapes were observed between the unoriented powder sample and the magnetically oriented sample.

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Flux Pinning Enhancement and Irreversibility Line of Sm doped YBCO Superconductor by Zone Melt Growth Process

  • Kim, So-Jung
    • Transactions on Electrical and Electronic Materials
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    • v.5 no.2
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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.

Effect of Mg Additive in the Bi1.84Pb0.34Sr1.91Ca2.03Cu3.06O10+δ(110 K phase) Superconductors (Bi1.84Pb0.34Sr1.91Ca2.03Cu3.06O10+δ(110 K 상)산화물 고온초전도체에 Mg 첨가에 따른 영향)

  • 이민수
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.16 no.6
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    • pp.522-531
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    • 2003
  • Samples with the nominal composition, B $i_{1.84}$P $b_{0.34}$S $r_{1.91}$C $a_{2.03}$C $u_{3.06}$ $O_{10+{\delta}}$ high- $T_{c}$ superconductors containing MgO as an additive were fabricated by a solid-state reaction method. Samples with MgO of 5~30 wt% each were sintered at 820~86$0^{\circ}C$ for 24 hours. The structural characteristics, critical temperature, grain size and image of mapping with respect to MgO contents were analyzed by XRD(X-Ray Diffraction), SEM(Scanning Electron Microscope) and EDS(Energy dispersive X-ray spectrometer) respectively. As MgO contents increased, intensity of MgO Peaks and ratio of Bi-2212 phase in superconductors intensified and the proportion of the phase transition from Bi-2223 to Bi-2212 was increased.

Hall Effect of High $T_{c}$ superconductor $Y_{1}Ba_{2}Cu_{3}O_{7-\delta}$ Thin Film (고온초전도체 $Y_{1}Ba_{2}Cu_{3}O_{7-\delta}$ 박막의 Hall 효과)

  • 허재호;류제천;김형국;김장환
    • Journal of the Korean Magnetics Society
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    • v.4 no.1
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    • pp.44-47
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    • 1994
  • High $T_{c}$ superconducting $Y_{1}Ba_{2}Cu_{3}O_{7-\delta}$ thin film was grown up for c-axis orientation by epitaxial growth method on $LaAlO_{3}$ single crystal substrate. The crystal structures of this thin film were found to be c-axis orientation by X-ray diffraction patterns. Hall effect and resistivity measurements were made by van der Pauw method. Hall resistivity was calculated from the magnetoresistivity by considering thermomagnetic effect. The relation was $pH=p_{s}tan{\alpha}_{n}-QBT\frac{S_s}{K_s}$ The measured Hall resistivity and the calculated one are in good agreement each other.

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