• Title/Summary/Keyword: HTS films

Search Result 63, Processing Time 0.018 seconds

Fabrication of a High-performance Oscillator with a Tunable High-Q HTS $YBa_2Cu_3O_{7-\delta}$ Resonator (High-Q $Yba_2Cu_3O_{7-\delta}$ 고온초전도체 공진기를 이용한 주파수 튜닝이 가능한 고성능 발진기 제작)

  • Yang Woo Il;Lee Jae Hun;Hur Jung;Lee Sang Young
    • Journal of the Institute of Electronics Engineers of Korea TC
    • /
    • v.42 no.7 s.337
    • /
    • pp.63-70
    • /
    • 2005
  • We investigated the phase noise of an oscillator with a extremely high-Q resonator used as the resonant element. A TE$_{011}$ mode rutile-loaded resonator with high-temperature superconductive (HTS) $YBa_2Cu_3O_{7-\delta}$(YBCO) films used as the endplates is prepared for this purpose. At 23.5 K, the unloaded Q and the loaded Q are 863000 and 180000, respectively. The phase noise of -104.8 dBc/Hz at 1 KHz offset was observed for the oscillator having a resonator with $Q_{L}$ =180000 at the $TE_{01\delta$ mode resonant frequency of 8.545 GHz at 23.5 K Such oscillators with very low phase noise are expected to be used for building up communication systems capable of efficient use of the frequency band and high-speed data transmission as well as for Doppler radars. Frequency tuning could be realized for the resonator by using a piezoactuator Applicability of the tunable rutile resonator for fabricating tunable oscillators of high performances is discussed.

Deposition of YBCO/BaZrO$_3$ films on MgO single crystal substrates by pulsed laser deposition (펄스레이저법으로 MgO 단결정 기판위에 YBCO/BaZrO$_3$ 박막의 증착)

  • Chung Jun-Ki;Ko Rock-Kil;Kim Hosup;Ha Hong-Soo;Song Kyu-Jeong;Moon Seung-Hyun;Yoo Sang-Im;Kim Cheol-Jin;Park Chan
    • Progress in Superconductivity and Cryogenics
    • /
    • v.6 no.3
    • /
    • pp.12-15
    • /
    • 2004
  • There are two major approaches to obtain texture template for HTS coated conductor (CC) ---IBAD and RABiTS. CC's with IBAD template showed both longer and higher Ic results so far. IBAD for CC began with YSZ, the processing of which is very slow compared to other processings needed for the fabrication of CC. Because of this very slow processing speed, IBAD with other materials such as Gd$_2$Zr$_2$O$_{7}$(GZO) and MgO have been developed. The processings of IBAD-GZO and IBAD-MgO are known to be up to 3times and 100 times. respectively, as fast as the processing of IBAD-YSZ. IBAD-MgO is very attractive in that the processing is very fast. IBAD-MgO also needs additional buffer layer(s). Many materials are being investigated to be used as a buffer layer on top of the MgO. BaZrO$_3$ (BZO) is a good candidate as the buffer layer on top of the IBAD-MgO because it is chemically stable and does not react with YBCO at high temperatures. It also has good lattice match with MgO. The BZO film has been deposited on single crystal MgO, and YBCO film was deposited on BZO/MgO to investigate the possibility of using BZO as both the buffer and capping layer of the CC.C.

Measurements of Correct Operation of a HTS 4-bit Shift Register Circuit (4-비트 고온초전도 Shift Register 회로의 동작 측정)

  • Park, Jong-Hyeog;Kim, Young-Hwan;Kang, Joon-Hee;Hahn, Taek-Sang;Kim, Chang-Hoon;Lee, Jong-Min;Choi, Sang-Sam
    • 한국초전도학회:학술대회논문집
    • /
    • v.9
    • /
    • pp.102-106
    • /
    • 1999
  • We have designed and fabricated a four-bit shift register circuit using YBCO bicrystal junctions and experimentally tested its operations by a computer-controlled digital measurement set-up. Laser ablated YBCO thin films with clean surface were used in this work. The circuit consists of the shift register and two read SQUIDs placed next to each sides of the shift register. The SQUIDs were inductively coupled to the nearby shift register stages. A probe equipped with high speed coax lines were used in this experiment. The major obstacle in testing the circuit was the interference between the read SQUIDs and we solved the problem by finding the correct operation points of the SQUIDs from the simultaneously measured modulation curves. Loaded Data("1" or "0") were successfully shifted from a stage to the next one by a controlled current pulse injected to the bias lines located between the stages and the data shifts were correctly monitored by the read SQUIDs

  • PDF