• Title/Summary/Keyword: CeO2 buffer layer

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Modeling and Simulation of the Delay Time in Superconductive Multi-pole Hairpin type Filter (Superconductive Multi-pole Hairpin type Filter과 Delay Time 설계 및 실험)

  • 양재라;정구락;강준희
    • Proceedings of the Korea Institute of Applied Superconductivity and Cryogenics Conference
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    • 2002.02a
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    • pp.135-137
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    • 2002
  • In the favor of adjusting microwave signal, Hairpin type Filter, which delay microwave signal enough to several nanosecond, is a key component. One of the main advantage in using Hairpin type Filter is a conveniency for equipping with Delay Module, and because of having a wide bandwidth, Hairpin type Filter can be designed to satisfy the most applications. In this work, we attempted to estimate the delay time in a superconductive hairpin type filter A software to synthesize even and odd order equiripple hairpin type filter has been developed. This software arbitrarily locate its transfer zeros making symmetric of asymmetric amplitude response and equalizing group delay. Borland C++ compiler has been used. The program was designed to run under MS-DOS, Window 98, Window 2000. The program optimizes the position of the transfer function zeros in order to fulfill the group delay specification masks. We designed and fabricated a hairpin type HTS 2-pole microstrip bandpass filter to operate at 5.8Ghz. The fabrication method was pulsed laser deposition and YBCO films were deposited on sapphire substrates with a Ce$O_{2}$ thin layer as a buffer layer. We also developed a new style hairpin type filter by using interdigitide inner-pole. Compared to the same size regular hairpin type filters, our filters had a lower center frequency.

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Meter-long coated conductor by R2R PVD methods on RABiTS template

  • Ko, Rock-Kil;Kim, Ho-Sup;Ha, Hong-Soo;Chung, Jun-Ki;Yang, Joo-Saing;Park, Yu-Mi;Shi, Dong-Qi;Song, Kyu-Jeong;Park, Chan;Yoo, Sang-Im;Moon, Seung-Hyun;Kim, Young-Cheol
    • Progress in Superconductivity and Cryogenics
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    • v.6 no.4
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    • pp.13-16
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    • 2004
  • Three film deposition systems (pulsed laser deposition, sputtering, and evaporation) equipped with reel-to-reel metal tape moving apparatus were installed and used to make meter-long coated conductor. Buffer architecture of $CeO_2/YSZ/Y_2O_3$ was deposited on Ni alloy using sputtering, evaporation, and PLD. YBCO superconducting layer was continuously deposited on buffered metal tape by PLD. End-to-end critical current ($I_c$) of 107 A at 77 K, self-field has been achieved in 1 em-wide tape (thickness 0.6∼1.0${\mu}{\textrm}{m}$, tape moving speed 54∼72 cm/hr) over 1 meter length.

Manufacturing of YBCO coated conductor deposited on RABiTS by pulsed laser deposition method (RABiTS 위에 PLD 방법으로 증착된 YBCO 초전도 박막 선재의 제조)

  • Ko Rock-Kil;Shi Dongqi;Chung Jun-Ki;Ha Hong-Soo;Kim Ho-Soup;Song Kyu-Jeong;Park Chan;Moon Seung-Hyun;Yoo Sang Im;Kim Young-Cheol
    • Progress in Superconductivity
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    • v.6 no.1
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    • pp.74-78
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    • 2004
  • YBCO coated conductor is one of the most promising materials as a new generations wire especially for practical power applications. In this work, $YBa_2$$Cu_3$$O_{7}$ -$\delta$/(YBCO) coated conductors (CC) were deposited by pulsed laser deposition (PLD) from buffer layers to superconducting layer on hi-axially textured metal tape. The oxide multilayer buffered substrate of architectures of $CeO_2$/$YSZ/Y_2$$O_3$ was fabricated by PLD at steady status. Then YBCO layer was deposited on RABiTS substrate by stationary and reel-to-reel (R2R) continuous process and we compared with deposition conditions of both processes. The degree of texture of each layer was investigated using X-ray diffraction including $\theta$-2$\theta$ scans, $\omega$-scans and $\Phi$-scans analysis. Their surface morphology was observed by scanning electron microscopy (SEM). The FWHM of the X-ray $\Phi$-scans and $\Phi$-scans indicated that YBCO and buffer layers closely replicate the in-plane and out-of-plane texture of metal tape. Critical current (Ic) at 77 K, self-field of 75.8 A/cm-width, critical temperature (Tc) of 85 K, and critical current density (Ic) of 3.7 MA/$\textrm{cm}^2$ were measured from coated conductor deposited by stationary process. And coated conductor deposited by R2R continuous process had Ic of 57.5 A/cm-width, Tc of 86.5 K and Jc of 2.0 MA/$\textrm{cm}^2$. The film also exhibits a homogeneous and dense surface morphology.

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The Study of a-Si Film Crystallization using an XeCl Laser Annealing on the Plastic Substrate

  • Kim, Do-Young;Suh, Chang-Ki;Shim, Myung-Suk;Kim, Chi-Hyung;Yi, Jun-Sin;Lee, Min-Chul;Han, Min-Gu
    • 한국정보디스플레이학회:학술대회논문집
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    • 2003.07a
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    • pp.634-638
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    • 2003
  • We reported the a-Si crystallization using a XeCl excimer laser annealing on the plastic substrate. The poly-Si film is able to grow in the low temperature and light substrate like a plastic. For the preparation of sample, substrate is cleaned by organic liquids. The film of $CeO_{2}$ layer as the buffer layer was grown by sputtering methods. After a-Si film deposition using ICPCVD, the film was crystallized by XeCl excimer laser. In this paper, we present the crystallization properties of a-Si on the plastic substrate

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Characterization of YBCO do SQUID fabricated on sapphire substrate for biomagnetic applications (생체자기 응용을 위한 사파이어 기판 위에 제작된 YBCO dc SQUID 의 특성)

  • Lim, Hae-Ryong;Kim, In-Seon;Kim, Dong-Ho;Park, Yong-Ki;Park, Jong-Chul
    • 한국초전도학회:학술대회논문집
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    • v.10
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    • pp.155-159
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    • 2000
  • YBCO step-edge dc SQUID magnetometers on sapphire substrates have been fabricated. CeO2 buffer layer and YBCO films were deposited in situ on the low angle (${\sim}$35$^{\circ}$) steps formed on the sapphire substrates. Typical 5-${\mu}$m-wide junction has R$_n$ of 5 ${\omega}$ and I$_c$ of 50 ${\mu}$A with large I$_c$R$_n$ product of 250 ${\mu}$V at 77K. According to applied bias current, depth of voltage modulation was changed and maximum voltage was measured 16 ${\mu}$V. Field noise of do SQUID was measured 100${\sim}$300 fT/${\surd}^{Hz}$ in the 1 $^{kHz}$, and about 1.5 pT/${\surd}^{Hz}$ in the 1/f region. For ac bias reversal method, field noise was decreased in the 1/f region. The QRS peak of magnetocardiogram was measured 50 pT in the magnetically shielded room.

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