• Title/Summary/Keyword: 초전도 박막

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마이크로파 응용을 위한 고온초전도 필터 서브-시스템

  • 강광용;김현탁;곽민환
    • The Proceeding of the Korean Institute of Electromagnetic Engineering and Science
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    • v.14 no.3
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    • pp.20-40
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    • 2003
  • Since unloaded Q-value of a high-temperature superconductor(HTS) filter is very high, a bandpass filter(BPF) and a lowpass filter(LPF) with an increase of pole numbers can be fabricated without an increase of an insertion loss(IL) ; recently a 70-pole BPF is developed in USA. They have an abrupt skirt property and an excellent attenuation level for out-of band. Moreover, they can be miniaturized when lumped element resonators or the slow-wave characteristic are used. Technology of fabricating a HTS epitaxial film as well as a film of a 4 inch area also makes the planar type filter with a various structure and an enhanced power handling capability possible. Recently, the HTS filter subsystems composed of a planar-type HTS filters, a GaAs-based LNA and a mini-cryocooler are developed. The extended receiver front- end subsystems for mobile radio communications decrease the noise-figure level of the communication system and the frequency interference interacted adjacent bands, and increase the efficiency of frequency and the capacity of communication system. In this paper, theory for developing the HTS filter, its kinds, its design rules, its characteristics are reviewed. The feature of the research and market trends related to the HTS filter systems for the receiver front-end subsystem of mobile base station are surveyed.

Characteristics of Co-deposition for Bi-superconductor Thin Film Using Ion Beam Sputtering Method (IBS 법으로 제작한 Bi 계 초전도 박막의 동시 증착 특성)

  • 박용필;이준웅
    • Electrical & Electronic Materials
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    • v.10 no.5
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    • pp.425-433
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    • 1997
  • BSCCO thin films have been fabricated by co-deposition at an ultralow growth rate using ion beam sputtering(IBS) method. The growth rates of the films was set in the region from 0.17 to 0.27 nm/min. MgO(100) was used as a substrate. In order to appreciate stable existing region of Bi 2212 phase with temperature and ozone pressure, the substrate temperature was varied between 655 and 82$0^{\circ}C$ and the highly condensed ozone gas pressure(PO$_3$) in vacuum chamber was varied between 2.0$\times$10$^{-6}$ and 2.3$\times$10$^{-5}$ Torr. Bi 2212 phase appeared in the temperature range of 750 and 795$^{\circ}C$ and single phase of Bi 2201 existed in the lower region than 785$^{\circ}C$. Whereas, PO$_3$dependance on structural formation was scarcely observed regardless of the pressure variation. And high quality of c-axis oriented Bi 2212 thin film with T$_{c}$(onset) of about 90 K and T$_{c}$(zero) of about 45 K is obtained. Only a small amount of CuO in some films was observed as impurity, and no impurity phase such as CaCuO$_2$was observed in all of the obtained films.lms.

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The Effect of Au nanoparticles on Critical current density of YBCO (Au 나노입자가 YBCO 전류밀도에 미치는 영향)

  • Oh, Se-Kweon;Jang, Gun-Eik;Kang, Byoung-Won;Lee, Cho-Yeon;Hyun, Ok-Bae
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.06a
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    • pp.191-191
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    • 2010
  • 초전도 전력 기기를 안정적으로 운용하기 위해서는 고자장하에서 높은 임계 전류 밀도($J_c$)를 지닌 초전도체 개발이 필수적이다. 최근 고자기장에서 전기적 특성을 향상시키는 방법으로는 YBCO 박막선재에 인위적 피닝센터로 고자장하에서도 $J_c$가 크게 증가 되었다고 보고되고 있다. 본 연구에서는 STO(100) 기판 위에 SAM 방법을 이용하여 금 나노분말을 분산시킨 후 PLD로 YBCO 박막을 증착하여 미세구조와 전기적인 특성을 분석하였다. 분산된 금 나노분말은 열처리전 나노입자의 높이는 29~32 nm, 지름은 41~49 nm툴 나타내었고 $800^{\circ}C$에서 진공 열처리 후에는 높이는 25~30 nm, 지름은 52~60 nm로 변형되었다. 임계온도는 순수 YBCO에서 85 K을 나타냈지만 금 나노입자를 적용한 YBCO의 경우는 80K으로 낮아진 것을 확인하였다. 임계전류밀도는 4T에서 측정된 경우 65 K에서는 순수한 YBCO는 141 KA/$cm^2$에서 금 나노입자가 형성된 기판에 증착한 YBCO는 42 KA/$cm^2$로 낮아졌다.

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Fabrication and characteristic analysis of High-Tc superconducting microstrip antennas using direct inset feeding technique (직접삽입 급전 방식을 이용한 고온초전도 마이크로스트립 안테나의 제작 및 특성 해석)

  • Chung, Dong-Chul;Han, Byoung-Sung;Kim, Jin;Ryu, Ki-Su;Hong, Suck-Yong;Lee, Jong-Ha
    • Journal of the Institute of Electronics Engineers of Korea TE
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    • v.37 no.1
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    • pp.70-78
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    • 2000
  • In applying high-${\underline{T_c}}$ superconducting material to microwave devices, Uncertainty of electromagnetics of high-${\underline{T_c}}$ superconductor(HTS) and the temperature dependence of the substrate fits with HTS thin film cause difficulty in realization of such antenna for industrial applications. It must be noted to characteristic the HTS antenna in contrast with normal conducting counterpart for this real application. In this paper, a comparative study between HTS microstrip antennas and gold antennas was reported in terms of the return loss, the characteristic impedance, efficiency, and other various characteristics. HTS thin films were $YBa_2Cu_3O_{7-x}$ (YBCO) on MgO substrates. Superconducting microstrip antennas used in this work were to directly inset a microstrip transmission line into the 50 ${\Omega}$ region of the radiating patch. Measurement results of HTS antennas and gold antennas showed that usable antennas can be made using this architecture.

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Non-invasive Measurements of the Thickness of YBCO Thin Films by Using Microwave Resonators: Roles of the Uncertainty in the Calibration Film Thickness (마이크로파 공진기를 이용한 YBCO 박막 두께의 비파괴적 측정: 캘리브레이션 박막 두께의 불확도의 역할)

  • Kim, Myung-Su;Jung, Ho-Sang;Yang, Woo-Il;Lee, Sang-Young
    • Progress in Superconductivity
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    • v.14 no.1
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    • pp.45-51
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    • 2012
  • Microwave metrology for the thickness of metallic or superconductive films provides a new way to measure the film thickness in a non-invasive way by using microwave resonators, with the measurement accuracy affected by standard uncertainties in the resonator quality factor, temperature-dependent resonant frequency and the dimensions of the resonators. Here we study effects of the standard uncertainty in the thickness, $t_{cal}$, of a calibration $YBa_2Cu_3O_{7-{\delta}}$ (YBCO) film on the measured thicknesses, $t_{RF}$, by using a ~ 40 GHz microwave resonator. For the study, we used five YBCO films having the thicknesses of 70 - 360 nm, for which relative standard uncertainties in $t_{RF}$ due to that in $t_{cal}$ are obtained. The standard uncertainty in $t_{cal}$ was determined with the surface roughness of the film taken into account. It appeared that relative standard uncertainty in $t_{cal}$ significantly affects the $t_{RF}$ values, with the values of 1% (5%) in the former resulting in those of 1-2% (5-9%) for the latter at 10 K. Our results show that, for realizing relative standard uncertainties less than 5% in $t_{RF}$ for all the YBCO films, the surface roughness of the calibration films should be small enough to realize a relative standard uncertainty of less than 2.7% in $t_{cal}$.

Pyroelectric Properties of the $\beta$-PVDF (Poly(vilnylidene fluoride)) Thin Film Prepared by Vacuum Deposition with Applying Electric Field (전계인가 진공 증착법으로 제작된$\beta$ -PVDF (Poly(vinylidene fluoride)) 박막의 초전 특성)

  • Chang, Dong-Hoon;Kang, Seong-Jun;Yoon, Yung-Sup
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.39 no.5
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    • pp.23-30
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    • 2002
  • The PVDF (Polyvinylidene Fluoride) thin film having P phase is prepared by the vacuum deposition with applying the electric field and its pyroelectric properties are studied by using a dynamic method to examine the possibility of the application to the pyroelectric IR sensor. The pyroelectric responses of the PVDF thin film are characterized as the frequency dispersion in both low and high modulation frequency regions, and their frequency dependences are observed. In the low frequency region (2~10Hzz), the polarization can easily rotate with the increase of modulation frequency and show the maximum since the reorientation rate of domains is higher than the modulation frequency. On the other hand, in the high frequency region (100~1000Hz), the pyroelectric response decreases as the frequency increases, because the reorienatation rate of domains is suppressed and thus, the change of polarization decreases. Pyroelectric coefficient, figure of merits for noise equivalent power and detectivity of the PVDF thin film are measured as 3.2$\times$10$^{-10}$ C/$\textrm{cm}^2$.K, 2.34$\times$10$^{-10}$ C.cm/J and 1.32$\times$10$^{-9}$ C.cm/J, respectively. Also, the noise equivalent and the detectivity are 1.66$\times$10$^{-7}$ W/H $z^{$\sfrac{1}{2}$}$, 6.03$\times$10$^{5}$ cm.H $z^{$\sfrac{1}{2}$}$W, respectively.

Study on deposition condition of epitaxial $Y_2O_3$ buffer layer deposited on textured metal substrates for $YBa_2Cu_3O_7$ coated conductors (YBCO Coated Conductor를 위한 texture된 금속 기판위의 epitaxial $Y_2O_3$ 완충층 증착 조건에 관한 연구)

  • Shin, K.C.;Ko, R.K.;Park, Y.M.;Chung, J.K.;Shi, Dongqi;Choi, S.J.;Song, K.J.;Park, C.;Son, Y.G.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2003.07a
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    • pp.565-568
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    • 2003
  • 2세대 초전도 선재로 알려져 있는 $YBa_2Cu_3O_{7-\delta}$ coated conductor는 금속모재/완충층/초전도층/보호층의 구조를 가진다. 2개 이상의 산화물 다층 박막으로 이루어진 완충층은 금속기판의 집합조직을 초전도층까지 전달하는 역할, 금속기판의 금속이 초전도층으로 확산되어 초전도층의 전기적 특성을 열화시키는 것을 막아주는 확산장벽으로의 역할 등을 수행한다. 1차 완충층은 금속기판의 집합조직을 유지하여야하며, 금속기판의 산화를 방지하면서 증착 되어야 한다. coated conductor 제조를 위한 첫 단계로 Pulsed Laser Deposition법을 이용하여 cube texture된 Ni 기판 위에 $Y_2O_3$ 박막을 증착 하였다. 최적의 증착 조건을 찾기 위해 증착 챔버의 산소 및 $H_2/Ar$ 혼합가스 분압과 기판온도를 변화시키면서 증착 하였다. $Y_2O_3$층의 (100) 집합조직은 기판온도 $600{\sim}700^{\circ}C$와 산소 분압 $0.01{\sim}0.1mTorr$에서 증착된 Y2O3 박막에서 금속기판과 유사한 집합조직을 얻을 수 있었다. 최적의 증착 조건에서 $Y_2O_3$ (222) ${\Phi}-scan$의 full width at half maximum (fwhm)이 $11^{\circ}$이고 (400) ${\omega}-scan$ fwhm은 $6^{\circ}$이었다.

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Thickness Effect on the Structural and Electrical Properties of YBCO Thin Films Grown by Pulsed Laser Deposition (PLD로 증착된 YBCO 박막의 두께에 따른 배향성과 전기적 특성 변화)

  • 허창회;한경보;이상렬
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2001.07a
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    • pp.617-619
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    • 2001
  • The effect of the superconducting film thickness on the substrate temperature has been investigated. Superconducting YBCO thin films have been grown on MgO substrates by pulsed laser deposition. The dependence of the orientation of YBCO film on thickness has been investigated by X-ray diffraction technique. X-ray diffraction indicated that the film orientation was changed by increasing the film thickness and by changing the substrate temperature.

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Deposition of YBCO and STO/YBCO thin films using ArF PLD system (ArF PLD System을 사용한 YBCO 박막과 STO/YBCO 박막의 제작)

  • Jung, Tae-Bong;Jang, Ju-Euk;Kang, Joon-Hee
    • 한국초전도학회:학술대회논문집
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    • v.9
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    • pp.43-47
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    • 1999
  • Instead of using KrF excimer lasers( ${\lambda}$ = 248 nm) in depositing oxide thin films, as in the most of the laboratories in Korea, we have used an ArF excimer laser( ${\lambda}$ = 197 nm) which has a shorter wavelength. By using a beam which has a shorter wavelength, we could obtain higher quality and smoother surface YBCO thin films. We fabricated YBCO thin films with the various substrate temperature conditions and analyzed the characteristics of these films. We also studied the charateristics of the films fabricated under the various conditions of the power of laser and the oxygen pressure. The characterization tools used in this work were a transport measurement setup, an XRD , and a SEM. We also fabricated STO/YBCO multilayers to use in SFQ devices fabrication. XRD patterns of the multilayers showed that the multilayer films were grown epitaxially.

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Uncooled pyroelectric thin-film (Ba,Sr)$TiO_3$ infrared detector thermally isolated by dielectric membrane (유전체 멤브레인에 의해 열 차단된 비냉각 초전형 박막 (Ba,Sr)TiO3 적외선 검지기)

  • Kim, Jin Seop;Lee, Jae Sin;Lee, Jeong Hui;Lee, Yong Hyeon
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.38 no.3
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    • pp.75-75
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    • 2001
  • Si₃N₄/SiO₂/Si₃N₄ 멤브레인에 의해 실리콘 기판으로부터 열차단된 비냉각 초전형 박막 (Ba,Sr)TiO₃ 적외선 검지기를 제작하고, 적외선 검지기의 특성을 논의하였다. 25℃의 공기중에서 쵸핑주파수가 1 ㎐일 때 적외선 검지기는 약 168.8 V/W의 비교적 높은 전압 감응도를 나타내었으나, 매우 작은 신호대잡음비 때문에 약 2.6×10⁴㎝·㎐/sup 1/2//W의 낮은 비검지도를 나타내었다. 또한 출력파형의 쵸핑주파수 및 온도 의존성에 대한 정성적인 해석으로부터 적외선 검지기의 열잡음전압 및 열시정수가 모두 상당히 크다는 것을 알 수 있었다.