• Title/Summary/Keyword: Superconducting transition

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High-Pressure Synthesis of $SmFeAsO_{1-x}F_x$(x=0.2) Single Crystals ($SmFeAsO_{1-x}F_x$(x=0.2)의 고압 단결정 합성)

  • Lee, Hyun-Sook;Park, Jae-Hyun;Lee, Jae-Yeap;Kim, Ju-Young;Cho, B.K.;Jung, Chang-Uk;Lee, Hu-Jong
    • Progress in Superconductivity
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    • v.10 no.2
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    • pp.87-91
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    • 2009
  • Fluorine-doped $SmFeAsO_{1-x}F_x$ single crystals with the nominal value of x=0.2 were grown at $1350-1450^{\circ}C$ under the pressure of 3.3 GPa by using the self-flux method. Plate-shaped single crystals in the range of a few-150 ${\mu}m$ in their lateral size were obtained. The detailed crystal structure was analyzed by using the x-ray diffractometry. Superconducting transition temperature, determined by the resistive transition, of a single crystal was about 49 K with a narrow resistive transition width of ${\sim}1$ K. A relatively sharp transition, a low residual resistivity, and a large residual resistivity ratio compared with those reported for $REFeAsO_{1-x}F_x$(RE=Sm, Nd) single crystals indicate the high quality of our single crystals.

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A Study of Joint Characteristic of BSCCO Superconductor Tape (BSCCO 고온초전도 선재의 접합특성 연구)

  • Kim, Jung-Ho;Kim, Joong-Seok;Kim, Tae-Woo;Ji, Bong-Ki;Joo, Jin-Ho;Nah, Wan-Soo
    • 한국초전도학회:학술대회논문집
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    • v.9
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    • pp.378-382
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    • 1999
  • We evaluated the effect of joining process such as contact method, shape of joined area and pressure on the electrical property of Bi-2223 superconducting tape. It was observed that the current capacity was reduced at the transition area of the joined tape and was significantly dependent on the uniaxial pressure. The lap-joined tape, fabricated with a pressure of 1,000-1,600 MPa, show the highest value of current capacity(80-90%) of the tape itself. It is believed the highest value of current capacity results from improvement in core density, contacting area and grain alignment, etc. In addition, the irreversible strain( ${\varepsilon}$ irrev) for the joined tape· was measured to be 0.1%, smaller than that of enjoined tape( ${\varepsilon}$ irrev = 0.3%). The decrease in the strength and irreversible strain for joined tape is believed to be due to the irregular geometry/morphology of the transition area of the tape.

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Angle-dependent modulation of the critical current of YBa$_2Cu_3O_7$ step-edge Josephson junctions on SrTiO$_3$ substrate (SrTio$_3$ 기판 위에 제작된 YBa$_2Cu_3O_7$ 계단형 모서리 조셉슨 접합의 각도에 따른 임계전류 특성)

  • Hwang, Yun-Seok;Moon, Sun-Kyung;Lee, Soon-Gul;Kim, Jin-Tae
    • 한국초전도학회:학술대회논문집
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    • v.9
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    • pp.83-86
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    • 1999
  • We have fabricated $_2Cu_3O_7$ step-edge junctions with different step orientations and studied their transition properties. Steps with different orientations were prepared on the substrate. Josephson junctions were made on a single substrate with step orientations ranging from 0$^{\circ}$ to 165$^{\circ}$ at 15$^{\circ}$ interval. We measured current-voltage characteristics, the critical current, and the superconducting transition temperature as a function of the angle. The critical current showed a modulation that has a maximum near 0$^{\circ}$ or 90$^{\circ}$ and a minimum near 45$^{\circ}$ and 135$^{\circ}$. We believe that the critical current modulation with the step orientation could be associated with the symmetry of high T$_c$ superconductor.

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Properties of $MgB_2$ Intragrain Nanobridges ($MgB_2$ 결정립 나노브릿지 특성에 관한 연구)

  • Hong, Sung-Hak;Lee, Soon-Gul;Seong, Won-Kyung;Kang, Won-Nam;Kim, Dong-Ho;Kim, Young-Kuk;Chung, Kook-Chae
    • Progress in Superconductivity
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    • v.10 no.2
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    • pp.74-78
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    • 2009
  • Inter-grain nanobridges of the $MgB_2$ superconductor have been fabricated by focused-ion-beam(FIB) and their electrical transport properties were studied. The $MgB_2$ film was prepatterned into microbridges by a standard argon ion milling technique and then FIB-patterned into 100 nm$\times$100 nm bridges. Current-voltage characteristics showed a strong flux-flow type behavior at all temperatures with a trait of Josephson coupling near $T_c$. At low temperatures, the curves showed a two-step resistance-doubled transition with occasional hysteresis. The resistance-doubling transition is believed to be due to a two-channel flux-flow effect. The temperature-dependent critical current data showed $I_c(T){\propto}(1-T/T_c)^2$ near $T_c$, same as a normal barrier junction, and $I_c(T){\propto}(1-T/T_c)^{1.2}$ at low temperatures, similar to that of a film.

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High Tc Superconductor Fiber $YBa_2Cu_3O_{7-{\sigma}}$ Synthesized by the Sol-gel Process (Sol-gel 법에 의한 고온 초전도체 $YBa_2Cu_3O_{7-{\sigma}}$ 선재 합성에 관한 연구)

  • Jin Ho Choy;Jong Seok Yoo;Bae Whan Kim;Seung Tae Hong
    • Journal of the Korean Chemical Society
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    • v.33 no.3
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    • pp.326-331
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    • 1989
  • Superconducting fiber of high Tc $YBa_2Cu_3O_{7-{\sigma}}$ was successfully prepared by the sol-gel method. The stoichiometric mixture of Y, Ba and Cu nitrates was dissolved in water, to which citric acid solution was added. Then ammonium hydroxide was added to the mixture in order to increase the pH to a value between 5.8 and 6.2. The mixture was heated carefully to form a homogeneous colloid sol at 358 K. The solution was viscous enough to draw a long gel fiber, which was then heated at 1223K for 8 hrs. under oxygen partial pressure of $Po_2$ = 1 atm., cooled slowly and annealed at 723K for 13 hrs.. The reacted superconducting sample maintained a fiber form with some shrinkage of its volume. The superconducting transition temperatures (Tc, onset and Tc, offset) of $YBa_2Cu_3O_{7-{\sigma}}$ have been determined to be approximately 95K and 82K, respectively. The superconducting phase was also confirmed by Meissner effect at liquid nitrogen boiling temperature.

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Effect of Cu substitution on Superconductivity in $(Ru_{1-x}Cu_x)Sr_2(Eu_{1.34}Ce_{0.66})Cu_2O_z$ System (Cu 치환에 따른 $(Ru_{1-x}Cu_x)Sr_2(Eu_{1.34}Ce_{0.66})Cu_2O_z$ 계의 초전도 특성)

  • Lee, H.K.
    • Progress in Superconductivity
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    • v.11 no.1
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    • pp.67-71
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    • 2009
  • The effect of Cu substitution on the structural and superconducting properties of the $(Ru_{1-x}Cu_x)Sr_2(Eu_{1.34{\cdot}}Ce_{0.66})Cu_2O_z$ system with x = 0, 0.25 and 0.5 prepared under ambient pressure have been investigated. The X-ray diffraction patterns indicated that the Ru ions are replaced by the Cu ions. It is found that the Cu substitution for Ru significantly reduces the ferromagnetic component of field-cooled magnetic susceptibility, but results in a small change in diamagnetic onset transition temperature of zero-field-cooled magnetic susceptibility. In contrast to the Ru $Sr_2(Eu_{1.34{\cdot}}Ce_{0.66})Cu_2O_z$, bulk Meissner effect is observed in the field-cooled magnetization measurements of the Cu doped samples. The experimental results are discussed in connection with the spontaneous vortex phase interpretation.

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Preparation and Characterization of Bi-Sr-Ca-Cu-O Superconductor Thin Film by Metal Organic Chemical Vapor Deposition (MOCVD법을 이용한 Bi-2212계 초전도박막 제조 및 특성에 관한 연구)

  • 장건익;김호인;박인길;김호기
    • Journal of the Korean Ceramic Society
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    • v.31 no.10
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    • pp.1123-1132
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    • 1994
  • Bi-Sr-Ca-Cu-O superconductor thin films were prepared on MgO and LaAlO3 substrates by MOCVD technique. The films deposited on MgO and LaAlO3 substrates became superconducting at 64 K and 70 K respectively. The measured critical current density of thin film deposited on LaAlO3 substrate was around 104 A/$\textrm{cm}^2$. After annealing at $700^{\circ}C$ for 3 hours, the critical transition temperature(Tc) of films deposited on LaAlO3 was changed from 70 K to 74 K.

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Deformation Mechanism Map for Creep and Superplastic Deformation in $YBa_2Cu_3O_{7-x}$ Ceramic Superconductors ($YBa_2Cu_3O_{7-x}$ 세라믹 초전도체의 크리프와 초소성변형에 대한 변형기관도)

  • 윤존도;초우예
    • Journal of the Korean Ceramic Society
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    • v.33 no.6
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    • pp.718-724
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    • 1996
  • Deformation mechanism map of Langdon-Mohammed type for YBa2Cu3O7-x superconducting ceramic was constructed by considering mechanisms of Nabarro-Herring Coble and powder-law creep and grain boundary sliding (GBS) with an accommodation by grain boundary diffusion. The map was found consistent with experi-mental results not only of the creep the also of the superplastic deformation. It showed the transition from interface reaction-controlled to the grain boundary diffusion-controlled GBS mechanism at about 1 ${\mu}{\textrm}{m}$ grain size and 100 MPa flow stress in agreement with the experimental results.

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Composition Control and Annealing Effects on the Growth of YBaCuO Superconducting Thin Films by RF Magnetron Sputtering (RF Magnetron Sputtering 방법에 의한 고온 초전도 박막 제조를 위한 조성 조절 및 열처리 효과)

  • 한택상;김영환;염상섭;최상삼;박순자
    • Journal of the Korean Ceramic Society
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    • v.27 no.2
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    • pp.249-255
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    • 1990
  • High Tc Supperconducting thin films were fabricated by rf magnetron sputtering method. We have successfully controlled the compositions of films by adding sintered CuO pellets on YBa2Cu3O7-x single target. High Tc thin films with large grian size and good crystal habit were obtained by rapid thermal annealing process. The films deposited on SrTiO3(100) single crystal substrate indicated the existence of c-axis prefered orientation confirmed by XRD and SEM analysis. The Tc, zero's of sharp resistive transition for rapid annealed films deposited on polycrystalline YSZ substrate and on SrTiO3(100) single crystal substrate were 79K and 88K, respectively.

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Fabrication of $Ba_{1-x}K_xFe_2As_2$ Thin Films in Various Conditions (다양한 조건에서의 $Ba_{1-x}K_xFe_2As_2$ 박막 제조)

  • Lee, Nam-Hoon;Jung, Soon-Gil;Kang, Won-Nam
    • Progress in Superconductivity
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    • v.12 no.1
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    • pp.32-35
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    • 2010
  • Potassium doped $BaFe_2As_2$ superconducting thin films by using an ex situ pulsed laser deposition technique were fabricated in various conditions to find out an optimal growth condition. Controlled conditions were annealing temperature, annealing time, and mass of potassium. The $Ba_{1-x}K_xFe_2As_2$ thin films which has most good quality is fabricated at a condition of annealing temperature at $700^{\circ}C$, annealing time of 60 minutes, and 0.6 g of potassium lumps. In this condition we were able to fabricate good quality films with high transition temperature of ~ 39 K.