• 제목/요약/키워드: High - T$_c$superconductor

검색결과 164건 처리시간 0.022초

구리 산화물 계열 초전도체에서의 스핀 요동에 의한 자체 에너지의 엘리아시버그 계산 (Eliashberg Calculation of the Momentum-Resolved Self-Energy for the Cuprate Superconductors Induced by the Spin Fluctuations)

  • 홍승환;최한용
    • Progress in Superconductivity
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    • 제13권3호
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    • pp.146-150
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    • 2012
  • We solve the momentum resolved d-wave Eliashberg equation employing the magnetic excitation spectrum from the inelastic neutron scattering on the LSCO superconductors reported by Vignolle et al. The magnetic excitation spectrum exhibits 2 peaks: a sharp incommensurate peak at 18 meV at momentum (${\pi}$, ${\pi}{\pm}{\delta}$) and (${\pi}{\pm}{\delta}$, ${\pi}$) and another broad peak near 40~70 meV at momentum (${\pi}$, ${\pi}$). Above 70 meV, the magnetic excitation spectrum has a long tail that is shaped into a circle centered at (${\pi}$, ${\pi}$) with ${\delta}$. The sign of the real part of the self-energy is determined by the momentum position of the peaks of the magnetic excitation spectrum and bare dispersion. We will discuss the effects of the each component of the magnetic excitation spectrum on the self-energy, the pairing self-energy.

외부자계 영향에 따른 HTS 선재의 직$\cdot$교류 통전 특성 (DC and AC current transport characteristics of HTS tapes with external magnetic field)

  • 임성우;최용선;최효상;황시돌;정영호
    • 한국초전도저온공학회:학술대회논문집
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    • 한국초전도저온공학회 2003년도 학술대회 논문집
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    • pp.15-18
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    • 2003
  • HTS(High Temperature Superconductor) tapes have dependence on critical characteristics such as electric, magnetic field and temperature. In order to confirm these effects, we examined the current transport characteristics of HTS tapes. First, after being fed DC and AC, the dependence of HTS tapes of 10cm on external magnetic field was investigated. On centeral region of HTS tape, about 1cm, external magnetic field was applied. Second, after applying DC of 50A to HTS tapes, we applied time variable magnetic field about 100mT and investigated the quench characteristics. Finally, AC, which is about 10 times of I$_{c}$, was applied to HTS tapes and over current characteristics were investigated. The data acquired in this study will be used as a source for the study of HTS cable conductor which is supposed to carry on.n.

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소형 초전도 부상자석의 특성 연구 (Study on the Characteristics of a Small Scale HTSC Levitation Magnet)

  • 조흥제;배덕권;이종민;고태국
    • 한국초전도ㆍ저온공학회논문지
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    • 제9권1호
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    • pp.76-81
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    • 2007
  • This paper deals with the characteristics of a small scale $high-T_c$ superconducting(HTSC) levitation system. The levitation tester. which models after electrodynamic suspension(EDS) maglev, consists of one HTSC magnet, a reaction plate, and force measuring components. Instead of moving magnet, AC current was applied to the fixed HTSC magnet. The magnet also has persistent current switch(PCS). The inductance of the magnet was 18.5 mH and total joint resistance of the magnet was $5.74{\times}10^{-7}\Omega$. AC current was applied into the HTSC magnet with various frequencies and the levitation force was calculated and measured. According to the increase of the vehicle speed, the levitation force was saturated.

S-parameter Circle-fit과 Lorentzian-fit 방법으로 측정된 고온초전도체 박막의 유효표면저항 비교 (A Comparative Study on the Effective Surface Resistance of High-$T_c$ Superconductor Films as Measured by Using the S-parameter Circle-fit and the Lorentzian-fit Methods)

  • 김민정;정호상;이재훈;이상영
    • Progress in Superconductivity
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    • 제9권2호
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    • pp.146-151
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    • 2008
  • Measurements of surface resistance ($R_s$) of high temperature superconductor (HTS) films with accuracy are essential for microwave applications of HTS materials. In using the dielectric resonator method, uncertainties in the unloaded quality factor of the resonator cause significant errors in the measured $R_s$ of HTS films. We compare the Rs values of $YBa_2Cu_3O_{7-{\delta}}$ films calculated from the $Q_0$ as determined from the Lorentzian fit with that from the $Q_0$ as determined from the S-parameter circle-fit at temperatures between 15 K and 77 K. The two sets of values appeared to differ by 5%, 7%, 6%, and 11% at temperatures of 15, 60, 70, and 77 K, respectively, from each other, implying that careful error analysis needs to be performed in obtaining the $R_s$ of HTS films by using the Lorentzian-fit method, with the ones determined from the S-parameter circle-fit used as the reference.

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수냉식 전기자로 구성된 1 MW 고온초전도 동기모터의 설계 (Design of 1 MW High-temperature Superconducting Motor with Water-cooled Armature)

  • 백승규;이재득;김석호;이언용;손명환;권영길;문태선;박희주;김영춘;이지영;홍정표
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2005년도 제36회 하계학술대회 논문집 B
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    • pp.1258-1260
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    • 2005
  • Superconducting synchronous motors and generators have the field coil composed of superconductor with almost zero resistance at superconducting state. Therefore, co or loss at the conventional field coil is eliminated and the superconducting machine gets higher efficiency. The armature coil of the superconducting machine is composed of cower wire and supported by non-magnetic material such as FRP(Fiber Reinforced Plastic). Although a fully-superconducting machine with superconducting armature coil has been researched, it was not developed toward industrial application because of AC transporting loss and difficulty in construction of the cooling structure and so on. This paper contains the design procedure of a 1 MW superconducting synchronous motor using high-temperature superconductor only for the field coil. Especially, the armature coil is designed by water-cooling in order to dissipate Joule heat easily. Moreover, 3-dimensional electromagnetic design is conducted to get a proper design result and reduce design errors from 2-dimensional approach.

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

  • 정동철;한병성;김진;유기수;홍석용;이종하
    • 대한전자공학회논문지TE
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    • 제37권1호
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    • pp.70-78
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    • 2000
  • 초전도체를 초고주파 소자에 응용하려고 할 경우, 초전도 전자기학의 불확실함이나 초전도 기판의 돈도 의존성은 산업 응용을 위한 안테나를 제작하는데 있어 어려움을 준다. 따라서 실제 응용을 위해서는 일반 안테나와 비교하여 정확하고 자세한 특성이 알려져야만 한다. 본 논문에서는 금 안테나와 초전도 안테나의 비교 연구를 수행하였으며 반사 손실, 특성임피던스, 효율 및 다른 다양한 특성들을 보고하였다. 본 연구에 사용된 고온초전도 박막은 $YBa_2Cu_3O_{7-x}$ (YBCO)/MgO 이며 초전도 안테나는 마이크로스트립 급전선을 방사 패치의 50 ${\Omega}$ 영역에 결합시키는 형태로 만들어졌다. 금 안테나와 초전도 안테나의 측정 결과는 이러한 구조를 이용하여 유용한 안테나가 제작될 수 있음을 보여주었다.

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Design of closed-loop nitrogen Joule-Thomson refrigeration cycle for 67 K with sub-atmospheric device

  • Lee, C.;Lee, J.;Jeong, S.
    • 한국초전도ㆍ저온공학회논문지
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    • 제15권1호
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    • pp.45-50
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    • 2013
  • Closed-loop J-T (Joule-Thomson) refrigeration cycle is advantageous compared to common open loop $N_2$ decompression system in terms of nitrogen consumption. In this study, two closed-loop pure $N_2$ J-T refrigeration systems with sub-atmospheric device for cooling High Temperature Superconductor (HTS) power cable are investigated. J-T cooling systems include 2-stage compressor, 2-stage precooling cycle, J-T valve and a cold compressor or an auxiliary vacuum pump at the room temperature. The cold compressor and the vacuum pump are installed after the J-T valve to create sub-atmospheric condition. The temperature of 67 K is possible by lowering the pressure up to 24 kPa at the cold part. The optimized hydrocarbon mixed refrigerant (MR) J-T system is applied for precooling stage. The cold head of precooling MR J-T have the temperature from 120 K to 150 K. The various characteristics of cold compressor are invstigated and applied to design parameter of the cold compressor. The Carnot efficiency of cold compressor system is calculated as 16.7% and that of vacuum pump system as 16.4%. The efficiency difference between the cold compressor system and the vacuum pump system is due to difference of enthalpy change at cryogenic temperature, enthalpy change at room temperature and different work load at the pre-cooling cycle. The efficiency of neon-nitrogen MR J-T system is also presented for comparison with the sub-atmospheric devices. These systems have several pros and cons in comparison to typical MR J-T systems such as vacuum line maintainability, system's COP and etc. In this paper, the detailed design of the subcooled $N_2$ J-T systems are examined and some practical issues of the sub-atmospheric devices are discussed.

1MW급 초전도 모터용 고온초전도 계자코일의 전자기적 특성 (Electromagnetic Characteristics of High-temperature Superconducting Field Coil for a 1MW class Superconducting Motor)

  • 백승규;손명환;이재득;이언용;권영길;문태선;박희주;김영춘;박관수
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2006년도 제37회 하계학술대회 논문집 B
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    • pp.661-662
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    • 2006
  • On the contrary of a conventional motor with very narrow air-gap, it is difficult to calculate the accurate magnetic field distribution and the performance of an air-cored superconducting motor by 2 dimensional analysis, which does not use high permeability material except outer machine shield. This paper aims to do analysis of magnetic field and force distribution from the 3 dimensional modelling of a 1MW class superconducting synchronous motor. Especially, the field coil composed of Bi-2223 high-temperature superconductor and the outer machine shield are modelled by finite element analysis software according to their structures and the self-inductance and Lorentz force are calculated based on the 3 dimensional magnetic field calculation.

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고온초전도 선재와 정합회로를 이용한 RF coil 제작에 대한 기초연구 (Study on fabricated RF coil using high-temperature superconductor tape and matching circuit for low field MRI system)

  • 김동혁;고락길;강부민;하동우;손명환;문치웅
    • 한국초전도ㆍ저온공학회논문지
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    • 제14권1호
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    • pp.44-47
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    • 2012
  • The substantial improvement of the signal-to-noise ratio (SNR) can be achieved with small-size samples or low-field MRI system by high-temperature superconducting(HTS) RF coil. The typical HTS RF coil made of HTS thin film is expensive and is limited the coil geometry to planar surface coil. In this study, commercial Bi-2223 HTS tapes was used as RF coil for a 0.35T permanent MRI system. It has advantages of both much lower cost and easier fabrication over HTS thin film coil. SNR gain of the image obtained from the HTS RF coil over a conventional Cu RF coil at room temperature was about 2.4-fold and 1.9-fold using the spin echo pulse sequence and gradient echo pulse sequence respectively.