• Title/Summary/Keyword: superconducting thin films

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Formation and Intergrowth of the Superconducting Phase in the Bi2Sr2Can-1CunOx (n=2~4) System

  • Cheon, Min-Woo;Park, Yong-Pil
    • Transactions on Electrical and Electronic Materials
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    • v.5 no.5
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    • pp.199-203
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    • 2004
  • Superconducting B $i_2$S $r_2$C $a_{n-l}$C $u_{n}$ $O_{x}$(n=2~4) thin films were prepared by single target DC-magnetron sputtering. And, that was compared with the B $i_2$S $r_2$C $a_{n-l}$C $u_{n}$ $O_{x}$(n=1~3) thin film fabricated by using the ion beam sputtering. Phase intergrowth among n=2-3, 3-4 and 4-5 phases was observed. The molar fraction of each phase in the mixed crystal of the deposited films was determined by x-ray diffraction analyses and investigated as a function of $O_2$ gas pressure during sputtering. We investigated the changes of the superconducting properties by molar fraction of each phase. Also, the thin film surface observation was carried out by atomic force microscope. The images show the average particle size decreases, and the distribution density of particles on the film surface was to increase with lower gas pressures. The fabrication conditions for selective growth of the single n=2, 3 and 4 phases in BiSrC $a_{n-l}$C $u_{n}$ $O_{x}$(n=2~4) thin film are discussed.e discussed.ussed.

Analysis of the Hi-system Superconducting Thin Films Fabricated by Layer-by-Layer Deposition Method at an Ultra low growth rate (초 저속 순차증착으로 제작한 Bi계 초전도 박막의 생성막 평가)

  • Yang, Seung-Ho;Kim, Young-Pyo;Park, Yong-Pil
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.06a
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    • pp.503-504
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    • 2007
  • $Bi_2Sr_2Ca_{n-1}Cu_nO_x$(n=0, 1, 2)superconducting thin films have been fabricated by atomic layer-by-layer deposition at an ultra low growth rate using IBS(Ion Beam Sputtering) method. During the deposition, 90 mol% ozone gas of typical pressure of $1{\sim}9{\times}10^{-5}$ Torr are supplied with ultraviolet light irradiation for oxidation. XRD and RHEED investigations reveal out that a buffer layer with some different compositions is formed at the early deposition stage of less than 10 units cell and then Bi-2201 oriented along the c-axis is grown.

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Fabrication Condition for Single Phase of Bi-superconductor Thin Film

  • Ahn, Joon-Ho;Park, Yong-Pil;Wang, Jong-Bae
    • Transactions on Electrical and Electronic Materials
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    • v.2 no.4
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    • pp.11-14
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    • 2001
  • Phase intergrowth in BSCCO thin films has been Investigated. It turfed out from XRD analyses of these phases that molar fraction of each constituent phase in the intergrowth thin film can be exhibited as a function of substrate temperature and ozone pressure. Super- conducting behavior of the intergrowth thin aim Is also discussed.

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Development of advanced laser processing for the fabrication of HTS metallic tapes for power applications (전력용 고온초전도 금속테이프 제작을 위한 첨단 레이저공정 개발)

  • Lee, Sang-Yeol
    • Proceedings of the KIEE Conference
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    • 1997.11a
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    • pp.688-691
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    • 1997
  • Good quality superconducting $YBa_2Cu_30_{7-{\delta}}$(YBCO) thin films were grown on Hastelloy (Ni-Cr-Mo alloys) with yttria-stabilized zirconia(YSZ) buffer layers by in situ pulsed laser deposition in a multi-target processing chamber. Generally, Hastelloy exhibits excellent resistance to corrosion, fatigue, thermal shock, impact, and erosion. However, it is difficult to make films on flexible metallic substrates due to interdiffusion problems between metallic substrates and superconducting overlayers. To overcome this difficulty, it is necessary to use YSZ buffer layer since it will not only limit the interdiffusion process but also minimize the surface microcrack formation due to smaller mismatch between the film and the substrate. In order to enhance the crystallinity of YBCO films on metallic substrates, YSZ buffer layers were grown at various temperatures different from the deposition temperature of YBCO films. On YSZ buffer layer grown at higher temperature than that for depositing YBCO film, the YBCO thin film was found to be textured with c-axis orientation by x-ray diffraction and had a zero-resistance critical temperature of about 85K.

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Characteristics of rapid-thermal-annealed $YBa_2Cu_3O_{7-x}$ high $T_c$, superconducting thin-films (급속 열처리에 의한 $YBa_2Cu_3O_{7-x}$ 고온 초전도체 박막의 특성)

  • Shin, Hyun-Yong;Park, Chang-Yub;Kim, Kyu-Soo
    • Proceedings of the KIEE Conference
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    • 1993.07b
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    • pp.1137-1139
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    • 1993
  • The superconducting thin films of $YBa_2Cu_3O_{7-x}$ were deposited on (100) sapphire substrates at low temperature by rf magnetron sputtering and annealed at $895^{\circ}C$ for 60 sec. using rapid-thermal-annealing(RTA) technique. The films were characterized by SEM, four-point probe resistivity measurement, XRD, and AES. The RTA processed HTS films had a preferential structure with c-axis normal to the substrate surface.

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Transport properties of polycrystalline TaNx thin films prepared by DC reactive magnetron sputtering method

  • Hwang, Tae Jong;Jung, Soon-Gil
    • Progress in Superconductivity and Cryogenics
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    • v.23 no.2
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    • pp.1-5
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    • 2021
  • We have investigated the electrical transport properties of polycrystalline tantalum nitride (TaNx) films. Various compositions of tantalum (nitride) thin films have been deposited on SiO2 substrates by reactive DC magnetron sputtering while changing the ratio of nitrogen partial pressure. The substrate temperature was maintained at 283 K during deposition. X-ray diffraction analyses indicated the presence of α-Ta and β-Ta phases in the Ta film deposited in pure argon atmosphere, while fcc-TaNx phases appeared in the sputtering gas mixture of argon and nitrogen. The N/Ta atomic ratio in the film increased ranging from 0.36 to 1.07 for nitrogen partial pressure from 7 to 20.7%. The superconducting transition temperatures of the TaNx thin films were measured to be greater than 3.86 K with a maximum of 5.34 K. The electrical resistivity of TaNx thin film was in the range of 177-577 𝜇Ωcm and increased with an increase in nitrogen content. The upper critical filed at zero temperature for a TaN0.87 thin film was estimated to exceed 11.3 T, while it showed the lowest Tc = 3.86 K among the measured superconducting TaNx thin films. We try to explain the behavior of the increase of the residual resistivity and the upper critical field for TaNx thin films with the nitrogen content by using the combined role of the intergrain Coulomb effect and disorder effect by grain boundaries.

Growth Model of Bi-Superconducting Thin Film Fabricated by Co-sputtering Method (동시 스퍼터법으로 제작한 Bi 초전도 박막의 성장 모델)

  • Chun, Min-Woo;Park, Yong-Pil
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2002.11a
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    • pp.796-799
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    • 2002
  • BSCCO thin films are fabricated via a co-deposition process at an ultra-low growth rate using ion beam sputtering. The sticking coefficient of Bi element exhibits a characteristic temperature dependence. This temperature dependence of the sticking coefficient was explained consistently on the basis of the evaporation and sublimation processes of Bi$_2$O$_3$.

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SI(superconductor-insulator) Transitions in Bi-superconducting Mixed Crystal Thin Films

  • Park, No-Bong;Yang, Sung-Ho;Park, Yong-Pil
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.07a
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    • pp.486-489
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    • 2002
  • Temperature(T) dependence of the sheet resistance( $R_{$\square$}$) has been investigated on the c-axis oriented thin films of the (Bi2212/Bi2201) mixed crystal with different molar fractions. The $R_{$\square$}$-T superconducting characteristic deteriorated with reduction of the Bi2212 fraction, and almost disappears at 48 mol% where a superconductor-to-insulator transition took place, with the resistance on the normal state, RN, reaching 4.l㏀ at 80 K. This $R_{N}$ value is close to the universal quantum number, h/(2e)$^2$≡6.5㏀ predicted by the Kosterlitz-Thouless(KT) transition theory. The $R_{$\square$}$-T characteristics of the 48 mol% thin film can be elucidated as a competitive process of KT transition brought about by charge or vortex in the two-dimensional layer structure.e.

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Terahertz time domain spectroscopy of GdBCO superconducting thin films

  • Ji, Gangseon;Park, Woongkyu;Lee, Hyoung-Taek;Song, Chang-Yun;Seo, Choongwon;Park, Minjo;Kang, Byeongwon;Kim, Kyungwan;Kim, Dai-Sik;Park, Hyeong-Ryeol
    • Progress in Superconductivity and Cryogenics
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    • v.21 no.1
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    • pp.15-17
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    • 2019
  • We present terahertz optical properties of $GdBa_2Cu_3O_{7-x}$ (GdBCO) superconducting thin films. GdBCO films with a thickness of about 105 nm were grown on a $LaAlO_3$ (LAO) single crystal substrate using a conventional pulsed laser deposition (PLD) technique. Using an Ar ion milling system, the thickness of the GdBCO film was reduced to 58 nm, and its surface was also smoothened. Terahertz (THz) transmission spectra through two different GdBCO films are measured over the range between 0.2 and 1.5 THz using THz time domain spectroscopy. Interestingly, the THz transmission of the thinner GdBCO film has been increased to six times larger than that of the thicker one, while the thinner film is still maintaining its superconducting property at below 90 K.

Substrate effects on the characteristics of $YBa_2Cu_3O_{7-x}$ thin films prepared by RF magnetron sputtering (RF마그네트론 스퍼터링법으로 제조한 $YBa_2Cu_3O_{7-x}$전도체 박막의 특성에 대한 기판의 영향)

  • 신현용;박창엽
    • Electrical & Electronic Materials
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    • v.8 no.1
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    • pp.6-12
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    • 1995
  • High Tc superconducting YBa$_{2}$Cu$_{3}$$O_{7-x}$ thin films were prepared on various substrates by off-axis rf magnetron sputtering method to examine the substrate effects on the film structure and its R-T characteristics. The SEM analysis showed that the surface morphology of the grown YBa$_{2}$Cu$_{3}$O.sub 7-x/, film has different characteristic structure with different substrate used. The film on (100) SrTiO$_{3}$ substrate has critical current density of 3*10$^{5}$ A/cm$^{2}$ at 77K under zero magnetic field. The X-ray diffraction measurements revealed that the films on (100) SrTiO$_{3}$ substrate have mixed a-axis and c-axis normal to the substrate surface and the films on (100) MgO and ZrO$_{2}$/sapphire substrates have c-axis normal orientation to the substrate surface. However, YBa$_{2}$Cu$_{3}$$O_{7-x}$ films on (100) sapphire substrates showed no preferential orientation.ion.

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