• 제목/요약/키워드: YBCO thin film

검색결과 177건 처리시간 0.019초

수정된 TFA-MOD법에 의한 (100) $SrTiO_3$ 단결정 기판 위 고 임계전류 밀도 $YBa_2Cu_3O_{7-{\delta}}$ 박막 제조 (Fabrication of high-$J_c$ $YBa_2Cu_3O_{7-{\delta}}$ thin films on (100) $SrTiO_3$ single crystal substrates by a modified TFA-MOD method)

  • 위성훈;신거명;송규정;홍계원;문승현;박찬;유상임
    • 한국초전도ㆍ저온공학회논문지
    • /
    • 제6권1호
    • /
    • pp.12-17
    • /
    • 2004
  • High critical current density. $J_c$ over $1MA/cm^2$ at 77 K in a self field was successfully achieved from the YBCO film prepared on (100) $SrTiO_3$ single-crystal substrates by the TFA-MOD process. Unlike a normal TFA-MOD process, we prepared the TFA precursor solution by dissolving YBCO powder into the trifluoroacetic acid. A significant amount of the second phases, including $BaF_2$, was observed in the films fired at $700-725^{\circ}C$ for 2 h under $P(O_2)=10^{-3}$ atm and $P(H_2O)=4.2%$, most probably due to an insufficient reaction time, and hence $T_c$ was greatly degraded. However the films fired at $750-800^{\circ}C$ for 2 h were composed of strongly c-axis oriented YBCO grams without any second phases. and exhibited the $T_c$ values of 89.5 ~ 91 K with a sharp transition. With increasing the firing temperature from 750 to $800^{\circ}C$ average grain size of YBCO was increased and grain connectivity was enhanced. The highest $J_c$ value of $1.1MA/cm^2$ was obtained from the YBCO film fired at $800^{\circ}C$.

펄스 레이저 증착법에 의한 금속기판상 초전도 박막의 증착 (Growth of superconducting thin film on metallic substrate by pulsed laser deposition)

  • 정영식;이상렬
    • 대한전기학회:학술대회논문집
    • /
    • 대한전기학회 1997년도 하계학술대회 논문집 C
    • /
    • pp.1298-1300
    • /
    • 1997
  • 금속기판상 초전도 $YBa_2CU_3O_{7-{\delta}}$ (YBCO) 박막을 yttria-stabilized zirconia (YSZ) 완충막을 이용하여 in situ 펄스 레이저 증착법에 의해 증착하였다. YBCO 박막을 직접 금속기판에 증착하게 되면 YBCO 박막과 금속기판 사이의 계면에서 상호확산현상이 발생하기 때문에 이를 방지하기 위해 YSZ 완충막이 사용되었다. YSZ 완충막의 증착온도가 박막의 결정성과 전기적 특성에 미치는 영향을 알아보기 위해 YSZ 완충막은 여러 가지 온도로 증착되었다. YBCO 박막의 증착온도와 같은 온도로 YSZ 완충막을 증착했을 때보다 YBCO 박막의 증착온도보다 높은 온도로 YSZ 완충막을 증착했을 경우, 증착된 YBCO 박막은 x선 회절에 의해 c 축 방향으로 성장하였음을 알 수 있었고, 저항이 0이 되는 임계온도가 83K가 되는 실험 결과를 얻었다.

  • PDF

마이크로파대에서의 강유전 박막 유전 특성 평가 (Characterization of Ferroelectric Thin Film in Microwave Region)

  • 박정흠
    • 한국전기전자재료학회논문지
    • /
    • 제17권10호
    • /
    • pp.1061-1067
    • /
    • 2004
  • In this study, ferroelectric (Ba,Sr)TiO$_3$ and high temperature superconductor YBCO thin films were fabricated by PLD (Pulsed Laser Deposition) method and tuneable bandstop filters were implemented with two different IDC(Interdigital Capacitance) gap patterns, 20${\mu}{\textrm}{m}$ and 30${\mu}{\textrm}{m}$ using these two thin film layers. The resonant frequency was changed by DC bias voltage. By comparing measured results with simulation, the dielectric properties of ferroelectric thin film have been extracted. The permittivity was 820 ~ 900 at 30 K and had an acceptable error range but the loss tangent had a great difference, 0.018 in 30${\mu}{\textrm}{m}$ IDC gap pattern and 0.037 in 20 ${\mu}{\textrm}{m}$.

YBCO 박막형 저항형 한류기에 적용 가능한 Meander Line 해석 연구 (Analytical Investigations on the Figures of Meander Lines on the YBCO Thin Film for Resistive Fault Current Limiters)

  • 이방욱;강종성;박권배;오일성;현옥배
    • 한국초전도저온공학회:학술대회논문집
    • /
    • 한국초전도저온공학회 2002년도 학술대회 논문집
    • /
    • pp.221-224
    • /
    • 2002
  • Superconducting electrical devices are under development in a national project in Korea. And KEPCO and LGIS are in charge of development of a resistive type fault current limiters(FCLs) with YBCO thin films. In order to realize FCLs, the rated power of FCLs must be increased. For this purpose, it is of great interest to increase of allowed voltage of unit component without electrical and thermal damages. So, meander lines were widely used for the conducting path to increase maximum electric field. In this research, numerical simulations on the electromagnetic behaviors of the device were carried out, especially focusing on the effect of meander line structures on the YBCO thin films. To evaluate the structures of meander lines, three types of meander lines were considered for numerical analysis using finite element method (FEM). In this simulation, both normal state and fault conditions were considered for calculation of electric field, current density, magnetic field density. And the simulation resulted are compared to find the optimum design of meander lines for resistive FCLs.

  • PDF

YBCO 박막을 이용한 3상 6.6kV 항형 초전도 한류기의 동시Quench 분석 (Simultaneous Quench Analysis of a Three-Phase 6.6 kV Resistive SFCL Based on YBCO Thin Films)

  • 심정욱;김혜림;현옥배
    • Progress in Superconductivity
    • /
    • 제6권1호
    • /
    • pp.46-51
    • /
    • 2004
  • We fabricated a resistive type superconducting fault current limiter (SFCL) of 3-phase $6.6 kV_{rms}$ / rating, based on YBCO thin films grown on sapphire substrates with a diameter off inch. Each element of the SFCL was designed to have the rated voltage of $600 V_{rms}$ $/35A_{rms}$. The elements produced a single phase with 8${\times}$6 components connected in series and parallel. In addition, a NiCr shunt resistor of 23 $\Omega$ was connected in parallel to each of them for simultaneous quenches between the elements. Prior to investigating the performance of the 3 phase SFCL, we examined the quench characteristics for 8 elements connected in series. For all elements, simultaneous quenches and equal voltage distribution within 10% deviation from the average were obtained. Based on these results, performance of the SFCL for single line-to-ground faults was investigated. The SFCL successfully limited the fault current of $10 kA_{ rms}$ below 816 $A_{peak}$ within 0.12 msec right after the fault occurred. During the quench process, average temperature of all components did not exceed 250 K, and the SFCL was totally safe during the whole operation.

  • PDF

HIGH TEMPERATURE SUPERCONDUCTING THIN FILMS PREP ARED BY PULSED LASER DEPOSITION

  • Park, Yong-Ki;Kim, In-Seon;Ha, Dong-Han;Hwang, Doo-Sup;Huh, Yun-Sung;Park, Jong-Chul
    • 한국표면공학회지
    • /
    • 제29권5호
    • /
    • pp.430-436
    • /
    • 1996
  • We have grown superconducting thin films on various substrates using a pulsed laser deposition (PLD) method. $YBa_2Cu_3O_7-\delta$ (YBCO) superconducting thin films with the superconducting transition temperature ($T_{c. offset}$) of 87K were grown on Si substrates using yittria-stabilized zirconia (YSZ) and $CeO_2$ double buffer layers. We have developed a large area pulsed laser deposition system. The system was designed to deposit up to 6 different materials on a large area substrate up to 7.5cm in diameter without breaking a vacuum. The preliminary runs of the deposition of YBCO superconducting thin films on $SrTiO_3$ substrate using this system showed a very uniform thickness profile over the entire substrate holder area. $T_{c}$ of the deposited YBCO thin film, however, was scattered depending on the position and the highest value was 85K.

  • PDF

질산염 전구체 원료로 분무 열분해 방법에 의한 YBCO 박막 증착 (Deposition of YBCO Thin Film by Aerosol Assisted Spray Pyrolysis Method using Nitrate Precursors)

  • 김병주;홍석관;김재근;이종범;이희균;홍계원
    • Progress in Superconductivity
    • /
    • 제12권1호
    • /
    • pp.68-73
    • /
    • 2010
  • Y123 films have been deposited on $LaAlO_3$ (100) single-crystal and IBAD substrates by spray pyrolysis method using nitrate precursors. Ultrasonic atomization was adopted to decrease the droplet size, spraying angle and its moving velocity toward substrate for introducing the preheating tube furnace in appropriate location. A small preheating tube furnace was installed between spraying nozzle and substrate for fast drying and enhanced decomposition of precursors. C-axis oriented films were obtained on both LAO and IBAD substrates at deposition temperature of around $710{\sim}750^{\circ}C$ and working pressures of 10~15 torr. Thick c-axis epitaxial film with the thickness of $0.3{\sim}0.6\;{\mu}m$ was obtained on LAO single-crystal by 10 min deposition. But the XRD results of the film deposited on IBAD template at same deposition condition showed that the buffer layers of the IBAD metal substrate was affected by long residence of metal substrate at high temperature for YBCO deposition.

위성 대 위성 통신용 광대역 HTS 안테나 제작 및 특성 해석 (Fabrication and Characterization of Wideband HTS Antennas for Satellite to Satellite Communication)

  • 정동철
    • 대한전기학회논문지:전기물성ㆍ응용부문C
    • /
    • 제51권12호
    • /
    • pp.573-577
    • /
    • 2002
  • We designed wideband HTS antennas which consists of two triangle -radiation patches using a $YBa_2Cu_3O_{7-X}$ (YBCO) superconducting thin film. The major limitation of high-Tc superconducting (HTS) microstrip antennas is the narrow bandwidth due to the high Q and thin substrate. Defining bandwidth as the frequency range over which standing wave ratio (SWR) 2:1 or less, HTS antenna bandwidths are typically 0.85 % to 1.1 %. Thus considerable effort has been focused on developing antennas for broadband operation. To calculate input impedance and design of the broadband HTS antennas a moment method technique was used. The HTS antenna fabricated in this work was designed for K-band, which is useful band for satellite to satellite communications. The bandwidth obtained was a significant 6.7 % and the other measured performance of our HTS antenna, including the bandwidth, radiation Pattern, efficiency, standing wave ratio (SWR) and return losses was reported.

위성 대 위성 통신용 광대역 HTS 안테나 제작 및 특성 해석 (Fabrication and Characterization of Wideband HTS Antennas for Satellite to Satellite Communication)

  • 정동철;최명호;황종선;강형곤;한병성
    • 한국전기전자재료학회:학술대회논문집
    • /
    • 한국전기전자재료학회 2002년도 하계학술대회 논문집
    • /
    • pp.523-526
    • /
    • 2002
  • We designed wideband HTS antennas which consists of two triangle-radiation patches using a YBa$_2$Cu$_3$O$\sub$7-x/ (YBCO) superconducting thin film. The major limitation of high-Tc superconducting (HTS) microstrip antennas is the narrow bandwidth due to the high Q and thin substrate. Defining bandwidth as the frequency range over which standing wave ratio (SWR) 2:1 or less, HTS antenna bandwidths are typically 0.85% to 1.1%. Thus considerable effort has been focused on developing antennas for broadband operation. To calculate input impedance and design of the broadband HTS antennas a moment method technique was used. The HTS antenna fabricated in this work was designed for K-band, which is useful band for satellite-to-satellite communications. The bandwidth obtained was a significant 6.7% and the other measured performance of our HTS antenna, including the bandwidth, radiation Pattern, efficiency, standing wave ratio (SWR) and return losses was reported.

  • PDF

DCA-MOD 방법으로 제조된 YBCO 박막의 미세조직에 미치는 열처리 효과 (Effects of Heat Treatments on the Microstructure of YBCO Films Prepared by DCA-MOD Method)

  • 김병주;김혜진;조한우;유석구;유정희;이희균;홍계원
    • Progress in Superconductivity
    • /
    • 제9권1호
    • /
    • pp.96-101
    • /
    • 2007
  • [ $YBa_2Cu_3O_{7-{\delta}}$ ] films have been prepared on $LaAlO_3$ (100) single-crystal substrates by a metalorganic deposition using dichloroacetate precursors (DCA-MOD). Calcination conditions were varied in order to optimize the microstructure and the superconducting properties of YBCO film. Coated films were calcined at various temperatures ranging from $400{\sim}700^{\circ}C$ in flowing humid oxygen atmosphere. Ramping rate to calcination tempertures was $2.22^{\circ}C/min$. Conversion heat treatment was performed at $800^{\circ}C$ for 2 h in flowing Ar gas containing 1000 ppm oxygen with a humidity of 9.45%. Observations of surface and cross sectional SEM microstructure showed that the particle size in the calcined film increased in the range of 100-200 nm with heating rate and the calcination temperature. SEM EDS analysis showed that 13 a/o of chlorine was contained in the calcined film. It was also observed that the porosity increased with the heating rate and temperature. Porous microstructure was developed when YBCO films were prepared using porous calcined film. Dense microstructure and high $J_c$ over $1\;MA/cm^2$ was obtained when calcination was carried out at the temperature of $500^{\circ}C$ with a heating rate of $2.22^{\circ}C/min$.

  • PDF