• Title/Summary/Keyword: $YBa_2Cu_3O_7$

Search Result 375, Processing Time 0.026 seconds

An automated measurement system for the microwave surface resistance of high-T$_c$ superconductor films

  • Lee, J.H.;Lim, J.;Lee, Jung-Hun;Lee, Sang-Young
    • 한국초전도학회:학술대회논문집
    • /
    • v.10
    • /
    • pp.173-178
    • /
    • 2000
  • A prototype for a highly sensitive, automated measurement system for the microwave surface resistance of high-T$_c$ superconductor films was set up, and tested by measuring the microwave surface resistances of high-T$_c$ YBa$_2$Cu$_3$O$_{7-{\delta}}$(YBCO) films at the frequency of about 19.6 GHz and the temperature of 30 K ${\sim}$ 90 K. An open-ended TE$_{011}$ mode sapphire-loaded cylindrical cavity resonator was used as the measurement probe, where YBCO films were used as the endplates of the cylindrical cavity. The characteristics of the measurement system include functions to display the unloaded ${\varrho}$ and the resonant frequency of the TE$_{011}$ mode resonator as well as the microwave surface resistance of the YBCO films, all simultaneously as a function of temperature. Applicability of the measurement system for investigating the homogeneity in the microwave properties of large high-T$_c$ superconductor films is discussed.

  • PDF

Fabrication of a HTS SQUID Magnetometer for Magnetocardiogram (심자도 측정용 고온초전도 SQUID magnetometer의 제작)

  • Kim, In-Seon;Lee, Sang-Kil;Kim, Jin-Mok;Kwon, Hyuk-Chan;Lee, Yong-Ho;Park, Yon-Ki;Park, Jong-Chul
    • Journal of Sensor Science and Technology
    • /
    • v.6 no.4
    • /
    • pp.258-264
    • /
    • 1997
  • $YBa_{2}Cu_{3}O_{7}$ single layer dc SQUID magnetometers, prepared on $1\;cm^{2}\;SrTiO_{3}$ substrates, have been fabricated and characterized. Based on the analytical description, a SQUID magnetometer design having a 8.5 mm pickup coil with 2.6 mm linewidth, and a SQUID inductance Ls = 50 pH with $3\;{\mu}m$ Josephson junctions is presented. The devices showed a maximum modulation voltage depth of $65\;{\mu}V$ and a magnetic field noise of 0.6 pT /$\sqrt{Hz}$ at 1 Hz. Clear traces of human magnetocardiogram could be obtained with the SQUID magnetometer operating at 77 K.

  • PDF

Effect of solvent on YBCO coated conductor prepared by MOD-TFA method (MOD-TFA방법으로 YBCO coated conductor 제조 시 용매의 영향)

  • 허순영;유재무;고재웅;김영국
    • Proceedings of the Korea Institute of Applied Superconductivity and Cryogenics Conference
    • /
    • 2003.10a
    • /
    • pp.87-89
    • /
    • 2003
  • YBa$_2$Cu$_3$$O_{7-x}$ thin films were fabricated by MOD-TFA process via dipping method on LaAlO$_3$(LAO) single crystalline substrates. In this study, we investigated effect of solvent on the microstructure and crystallinity of YBCO thin films. The YBCO films derived from solvent with low boiling point has good surface morphologies.s.

  • PDF

Comparative Study on the Fabrication of Single Grain YBCO Bulk Superconductors using Liquid Infiltration and Conventional Melt Growth Processes (단결정 YBCO 벌크 초전도체 제조에 대한 액상침투법과 고전적 용융공정의 비교연구)

  • Mahmood, Asif;Jun, Byung-Hyuk;Kim, Chan-Joong
    • Progress in Superconductivity
    • /
    • v.11 no.1
    • /
    • pp.42-46
    • /
    • 2009
  • With an aim of comparison, single grain Y-Ba-Cu-O (YBCO) bulk superconductors were fabricated using a liquid infiltration growth (LIG) process and a conventional melt growth (MTG) process with top seeding. The MTG process uses an $YBa_2Cu_3O_{7-x}$(Y123) powder as a precursor, while the LIG process uses $Y_2BaCuO_5(Y211)/Ba_3Cu_5O_8(Y035)$ pre-forms. The growth of a single Y123 domain on the top seed was successful in the both processes. Different feature between the two processes is the interior microstructure regarding the critical current density ($J_c$). The LIG-processed YBCO sample showed a lower porosity, more uniform distribution of Y211 particles and the enhanced Y211 refinement compared to the conventional MTG process. The $J_c$ improvement in the LIG process is attributed to the dispersion of finer Y211 particles as well as lower porosity within the Y123 superconducting matrix.

  • PDF

Preparation of a axis oriented $YBa_2Cu_3O_{7-\delta}$ thin films by RF magnetron sputtering (RF 마그네트론 스퍼터링법에 의한 a-축 배향 $YBa_2Cu_3O_{7-\delta}$박막의 제조)

  • Lee, J.J.;Kim, Y.H.;Shin, J.;Lee, K.H.;Choi, S.S.;Hahn, T.S.
    • Korean Journal of Materials Research
    • /
    • v.4 no.4
    • /
    • pp.459-465
    • /
    • 1994
  • A-axis oriened YBCO thin flims were grown on $LaAIO_{3}$ single crystal substrate by off-axis rf magnetron sputtering method. We used two kinds of process to get a-axis oriented fi1ms;one-step process and two-step process. In one-step process, films are grown in single step in which substrate temperature( $T_s$) is in the range of $590^{\circ}C$ to $680^{\circ}C$. On the other hand, in two step process a-axis oriented thin film templates i f about 30nm thickness is deposited at low temperature first, and subsequently films are grown at elevated temperature to the final thickness of about 100nm. In the case of one step process($T_s$ ~)$600^{\circ}C$), prefered a-axis orientation is dominant and Cu-rich phases segregate at the surface. Segregations decrease and ($00 \ell$) peaks increase upon increasing $T_s$. The films prepared by two step method appeared to have strong(h00) peaks as the deposition rate increased. Microstructure shows pin holes resulted from mixed phases of a-axis and c-axis oriented films. In both cases of one step and two step process, as TS decreases, prepared films show stronger a-axis orientation. However electrical properties of the films are depressed with lower $T_c$ and wider $\Delta T$ as $T_s$ decreases.

  • PDF

Fabrication of YBCO films on metal tapes by the TFA-MOD process (TFA-MOD법에 의한 금속기판 위 YBCO 박막 제조)

  • Shin Geo-Myung;Song Kyu-Jung;Park Chan;Moon Seung-Hyun;Yoo Sang-Im
    • Progress in Superconductivity
    • /
    • v.7 no.1
    • /
    • pp.92-96
    • /
    • 2005
  • YBCO thin films on metal substrates were prepared by the metal-organic deposition using trifluoroacetates (TFA-MOD). To compensate the loss of Ba element from the precursor films due to the reaction with $CeO_2$ cap layer, we have employed Ba-excessive precursor solutions of $YBa_{2+x}Cu_{3}O_{7-{\delta}}$ ($0{\le}x{\le}0.1$). The precursor solutions were dip-coated on the metal substrates with $CeO_2$ cap layer, initially heated up to $400^{\circ}C$, and finally fired at the various high temperatures for 2 h in a reduced oxygen atmosphere. With this approach, YBCO films possessing critical temperature over 85 K could be successfully prepared on the metal substrates. The highest $T_{c,zero}$ value of 86 K was obtained from the Ba-excessive YBCO film of x=0.005 in $YBa_{2+x}Cu_{3}O_{7-{\delta}}$ fired at $750^{\circ}C$ for 2 h. However, unexpected $T_c$ suppression even in Ba-excessive YBCO samples requires further identification.

  • PDF

펄스 레이저를 이용한 고온 초전도박막 증착의 레이저-타깃 반응 기구

  • Seo, Jeong-Dae;Gang, Gwang-Yong;Seong, Geon-Yong
    • Electronics and Telecommunications Trends
    • /
    • v.7 no.3
    • /
    • pp.84-95
    • /
    • 1992
  • 본 고에서는 $YBa_2Cu_3O_7_x$ 고온초전도 물질의 박막제조에 있어서 현재 가장 각광을 받고 있는 펄스 레이저 증착공정의 원리, 특징등을 살펴보았다. 특히, 이 공정에서 입사 레이저와 고체 타깃간의 상호작용으로 인한 플룸의 발생, 물질의 방출, 기판상의 증착 등과 관련된 반응기구를 중점적으로 기술하였다.

Interface Characterization of Supeconducting Thin Film on Sapphire Grown by an Excimer Laser (액시머 레이저로 증착된 초전도박막과 사파이어 기판간 계면 특성 분석)

  • 이상렬;박형호;강광용
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
    • /
    • 1995.11a
    • /
    • pp.148-151
    • /
    • 1995
  • Excimer laser has been used to fabricate superconducting YBa$_2$Cu$_3$O$\sub$7-x/(YBCO) thin films on various substrates. An XeCl excimer laser with an wavelength of 308 nm was used to deposit both buffer layer and superconducting thin film on sapphire substrate. The characterizations of the interface between thin film and substrate were performed. The interfacial properties of thin films on buffered sapphire and on bare sapphire were compared. With a 20 nm PrBa$_2$Cu$_3$O$\sub$7-x/(PBCO) buffer layer, no diffusion layer was observed between film and substrate while the diffusion layer with about 30 nm thickness was observed between film and sapphire without buffer layer.

  • PDF