• Title/Summary/Keyword: TFA process

Search Result 56, Processing Time 0.027 seconds

Optimization of annealing conditions in oxide-precursor-based MOD process for YBCO thin films (산화물 전구체를 이용한 YBCO 박막제조에서 열처리조건의 최적화)

  • Heo S. Y.;Kim Y. K.;Yoo J. M.;Ko J. W.;Hong G. W.;Lee H. G.;Yoo S. I.
    • Progress in Superconductivity
    • /
    • v.6 no.2
    • /
    • pp.118-123
    • /
    • 2005
  • A low cost YBCO oxide powder was employed as a starting precursor for MOD process. YBCO oxide is advantageous over metal acetates or TFA salts which are popular starting precursors for conventional MOD-TFA process because that YBCO oxide precursor is cheap and easy to control molar ratio. YBCO thin films were prepared by this oxide-precursor-based MOD process and annealing condition was optimized. The YBCO thin film annealed at below $780^{\circ}C$ shows no transport $I_c$ and poor microstructure. Raman spectroscopic study of YBCO thin film indicates that YBCO thin film prepared at below $780^{\circ}C$ contains a number of imperfections such as non-superconducting $BaCuO_2$ phase, cation disorder, etc. However, the YBCO thin film treated at above $800^{\circ}C$ shows improvement in microstructure and current transport properties. This research was supported by a grant from Center for Applied Superconductivity Technology of the 21st Century Frontier R&D Program funded by the Ministry of Science and Technology, Republic of Korea.

  • PDF

New processing technique of TFA-MOD YBCO coated conductors using the '211' process (211 공정을 이용한 새로운 TFA-MOD YBCO 박막 선재 제조)

  • Lim, Jun-Hyung;Jang, Seok-Hern;Kim, Kyu-Tae;Lee, Jin-Sung;Yoon, Kyung-Min;Park, Eui-Cheol;Joo, Jin-Ho
    • Progress in Superconductivity
    • /
    • v.7 no.2
    • /
    • pp.140-144
    • /
    • 2006
  • We fabricated the YBCO films on single crystal $LaAlO_3$ substrates via a metal organic deposition (MOD) process. In the process, $Y_2Ba_1Cu_1O_x$ and $Ba_3Cu_5O_8$ powders were dissolved in trifluoroacetic acid (TFA) followed by calcining and firing heat treatments. To evaluate the effects of the firing temperature on YBCO phase formation and critical properties, the films were fired at $750^{\circ}C,\;775^{\circ}C\;and\;800^{\circ}C$ after calcining at $430^{\cric}C$. Microstructure observation indicated that a crack-free surface formed and a strong biaxial texture was developed. The FWHM of out-of-plane texture was measured to be in the range of $4.3^{\cric}-7.0^{\circ}$ for all the films. When the YBCO film was fired at $775^{\cric}C$, it had the highest critical properties: 88.5 K of critical temperature and 16 A/cm-width of critical current ($1MA/cm^2$ as critical current density). On the other hand, those properties were degraded as firing at $750^{\circ}C\;and\;800^{\circ}C$. It is considered that the improved critical values are partly owing to dense and homogeneous microstructure, strong texture, and high oxygen content.

  • PDF

Effect of chemically modified precursor solution on MOD-processed YBCO thin films

  • Jaimoo Yoo;Kim, Young-Kuk;Jaewoong Ko;Soonyoung Heo;Hyungsik Chung
    • Progress in Superconductivity and Cryogenics
    • /
    • v.5 no.3
    • /
    • pp.23-25
    • /
    • 2003
  • Effect of chemically modified precursor solution on YBCO coated conductor prepared by MOD-TFA method was investigated. YBCO thin films were deposited on (l00)-oriented single crystalline LaAlO$_3$ substrates by conventional MOD-TFA process. The microstructures of YBCO thin films contain maze-like patterns. The origin of this microstructure was delineated by compositional inhomogeneity during the pyrolysis process and it was shown that addition of diethanolamine (DEA) improve the microstructure of grown YBCO films. In addition, it was demonstrated that the chemical modification of precursor solution makes no harmful effect on biaxial texture of YBCO thin films.

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

Microstructural Observation of Multi-coated YBCO Films Prepared by TFA-MOD (TFA-MOD법으로 제조된 다층 YBCO 박막의 미세구조 관찰)

  • Jang, Seok-Hern;Lim, Jun-Hyung;Lee, Chang-Min;Hwang, Soo-Min;Choi, Jun-Hyuk;Shim, Jong-Hyun;Joo, Jin-Ho;Kim, Chan-Joong
    • Progress in Superconductivity
    • /
    • v.9 no.2
    • /
    • pp.167-172
    • /
    • 2008
  • We fabricated $YBa_2Cu_3O_{7-x}$(YBCO) films on (00l) $LaAlO_3$ substrates prepared by metal organic deposition(MOD) method using trifluoroacetate(TFA) solution. The films with various thicknesses were prepared by repeating the dip-coating and calcining processes. The effects of film thickness on phase formation, microstructures, and critical properties were evaluated by X-ray diffraction, scanning electron microscopy, and transmission electron microscopy. The microstructure and resultant critical current($I_C$) and critical current density($J_C$) varied remarkably with film thickness: The ($I_C$) value increased from 39 to 160 A/cm-width as the number of coatings increased from one to four, while the corresponding $J_C$ was measured to be in the range of $0.84-1.21\;MA/cm^2$. Both the $I_C$ and $J_C$ decreased when an additional coating was applied due to microstructural degradation, indicating that the optimum thickness is in the range of $1.1-1.8\;{\mu}m$. The possible cause for the decrease in the $I_C$ and $J_C$ value for film thicker than $1.8\;{\mu}m$ include non-uniform thickness, increased surface roughness, and the poor formability of the YBCO phase and texture arising from the insufficient heat treatment time with respect to the increased thickness.

  • PDF

Effects of the Heat Treatment Temperature and Thickness of YBCO Film Fabricated by TFA-MOD Method (TFA-MOD법을 이용한 YBCO 박막의 열처리 온도와 두께의 영향)

  • Jang Seok-Hern;Lim Jun-Hyung;Lee Jin-Sung;Yoon Kyung-Min;Kim Kyu-Tae;Joo Jin-Ho;Kim Chan-Joong;Nah Wan-Soo
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
    • /
    • v.19 no.5
    • /
    • pp.467-476
    • /
    • 2006
  • We fabricated the YBCO films on LAO substrate using the TFA-MOD method and evaluated the effects of heat treatment temperature and film thickness on the microstructure, degree of texture, and critical properties. The calcining and firing were peformed at the temperature range of $370^{\circ}C-460^{\circ}C\;and\;750^{\circ}C-800^{\circ}C$, respectively. For the films fired at $775^{\circ}C$ after calcining at $400^{\circ}C-430^{\circ}C$showed highest critical temperature (Tc-onset) of 89.5 K and critical current (Ic) of 40A/cm-width which corresponds to critical current density (Jc) of $1.8MA/cm^2$. The highest critical properties are probably attributed to the formation of purer YBCO phase, stronger biaxial texture, and higher oxygen content, according to the XRD, pole-figure, SEM, Raman analysis. From the multi-coated films, the Ic increased from 39 to 169 A/cm-width as the coating repeated to four times, while the corresponding Jc was measured from once to be in the range of $0.8-1.2MA/cm^2$. Both Ic and Jc degraded as the coating repeated further, indicating that the optimum thickness is in the range of $1.0{\mu}m-1.7{\mu}m$.