• Title/Summary/Keyword: MgB2 thin films

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Origin of High Critical Current density in $MgB_2$ thin films

  • Kang, W.N.;Kim, Hyeong-Jin;Park, Eun-Mi;Kim, Mun-Seong;Kim, Kijoon H. P.
    • Progress in Superconductivity
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    • v.3 no.2
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    • pp.135-139
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    • 2002
  • We have fabricated high-quality c-axis-oriented $MgB_2$ thin films by using a pulsed laser deposition technique. The thin films grown on (1 1 0 2) $Al_2$$O_3$ substrates show an onset transition temperature of 39.2 K with a sharp transition width of ~0.15 K. X-ray diffraction patterns indicate a c-axis-oriented crystal structure perpendicular to the substrate surface. We observed high critical current densities ($J_{c}$) of ~ 16 $MA/\textrm{cm}^2$ at 15 K and under self-field, which is comparable to or exceeds those of cuprate high-temperature superconductors. The extrapolation $J_{c}$ at 5 K was estimated to be ~ 40 MA/$\textrm{cm}^2$, which is the highest record for $MgB_2$ compounds. At a magnetic field of 5 T, the $J_{c}$ of~ 0.1 $MA/\textrm{cm}^2$ was detected at 15 K, suggesting that this compound is very promising candidate for the practical applications at high temperature with lower power consumption. As a possible explanation for the high current-carving capability, the vortex-glass phase will be discussed.d.d.d.

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Mixed-state Hall effect of $MgB_2$ thin films ($MgB_2$박막의 혼합상태에서의 홀 효과)

  • Kim, Bo-Yeon;Jung, Soon-Gil;Moon, Kyeong-Hee;Kang, W.N.;Choi, Eun-Mi;Kim, Heon-Jung;Lee, Sung-Ik;Kim, Hyeong-Jin
    • Progress in Superconductivity
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    • v.7 no.2
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    • pp.103-108
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    • 2006
  • We have measured the Hall resistivity (${\rho}_{xy}$) and the longitudinal resistivity (${\rho}_{xy}$) on superconducting $MgB_2$ thin films in extended fields up to 18 T. We found a universal scaling behavior between the Hall resistivity and the longitudinal resistivity, which is independent of the temperature and the magnetic field. At a wide magnetic field region from 1 to 18T, a universal power law of ${\beta}=2.0{\pm}0.1$ in a scaling relation, ${\rho}_{xy}={A{\rho}_{xx}}^{\beta}$, was observed in c-axis-oriented $MgB_2$ thin films. These results can be well interpreted by using recent models.

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Bi2Sr2CaCu2O8+d Thin Films Grown on (100) MgO Substrate by Metallorganic Decomposition Method (MOD 방법을 이용한 Bi2Sr2CaCu2O8+d 박막제작)

  • ;;;;Takayuki Ishibashi;Katsuaki Sato
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.16 no.11
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    • pp.1035-1040
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    • 2003
  • High $T_{c}$ superconducting B $i_2$S $r_2$CaC $u_2$ $O_{8+d}$ (BSCCO2212) films were prepared by a metallorganic decomposition (MOD) method. The metal organic solution of BSCCO2212 was spin-coated on MgO (100) substrates at 3000 rpm for 1 min. To achieve a high critical current density, we controlled heat-treatment conditions and atmosphere. The films were annealed at temperature 75$0^{\circ}C$ ∼ 80$0^{\circ}C$ in $O_2$ or air. We obtained c-axis orientated BSCCO thin films on MgO substrates. The annealed sample at 77$0^{\circ}C$ with $O_2$ showed the critical temperature about 77 K and critical current denstity of 1.19 ${\times}$ 10$^{5}$ A/$\textrm{cm}^2$ about 13 K.

High density plasma etching of MgO thin films in $Cl_2$/Ar gases

  • Xiao, Y.B.;Kim, E.H.;Kong, S.M.;Chung, C.W.
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.02a
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    • pp.213-213
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    • 2010
  • Magnetic random access memory (MRAM), based on magnetic tunnel junction (MTJ) and CMOS, is one of the best semiconductor memories because it can provide nonvolatility, fast access time, unlimited read/write endurance, low operating voltage and high storage density. For the realization of high density MRAM, the etching of MTJ stack with good properties is one of a key process. Recently, there has been great interest in the MTJ stack using MgO as barrier layer for its huge room temperature MR ratio. The use of MgO barrier layer will undoubtedly accelerate the development of MTJ stack for MRAM. In this study, high-density plasma reactive ion etching of MgO films was investigated in an inductively coupled plasma of $Cl_2$/Ar gas mixes. The etch rate, etch selectivity and etch profile of this magnetic film were examined on vary gas concentration. As the $Cl_2$ gas concentration increased, the etch rate of MgO monotonously decreased and etch slop was slanted. The effective of etch parameters including coil rf power, dc-bais voltage, and gas pressure on the etch profile of MgO thin film was explored, At high coil rf power, high dc-bais voltage, low gas pressure, the etching of MgO displayed better etch profiles. Finally, the clean and vertical etch sidewall of MgO films was achieved using $Cl_2$/Ar plasma at the optimized etch conditions.

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Effect of Deposition Rate on $MgB_2$ Thin Films Growth by Co-deposition Method (동시증착법에 의해 성장된 붕화마그네슘 박막의 증착속도에 따른 효과)

  • Park, Sung-Chang;Kang, Seong-Gu;Jeong, Dae-Gil;Chung, Jun-Ki;Lim, Yeong-Jin;Kim, Chan-Joong;Kim, Cheol-Jin
    • Progress in Superconductivity
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    • v.10 no.1
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    • pp.29-34
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    • 2008
  • Magnesium diboride ($MgB_2$) is an inexpensive and simple superconductor. This material was first synthesized and its structure confirmed in 1953 but its superconducting properties were not discovered until 2001 when they caused great excitement. In this study, superconducting $MgB_2$ thin films on the r-$Al_{2}O_3$ substrates have been grown by the combination of radio frequency magnetron sputtering of B and thermal evaporation of Mg. The deposition conditions were varied by changing deposition rate. Before the co-deposition of Mg and B, the deposition rates of each element have been measured separately. The $MgB_2$ layers had 400nm in thickness and superconducting transition temperatures have been measured around $\sim$38.6K. Superconducting properties have been measured by PPMS, XRD, and SEM.

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Characteristics of c-axis oriented PLT thin films and their application to IR sensor (c-축 배양된 PLT 박막의 특성 및 IR센서 응용)

  • Choi, B.J.;Park, J.H.;Kim, Y.J.;Kim, K.W.
    • Journal of Sensor Science and Technology
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    • v.5 no.3
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    • pp.87-92
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    • 1996
  • The PLT thin films on (100) cleaved MgO single crystal substrate have been fabricated by rf magnetron sputtering using a PbO-rich target. The dependence of physical and electrical properties on the degree of c-axis orientation has been studied. The degree of c-axis orientation of PLT thin films depends on fabrication conditions. Fabrication conditions of the PLT thin films were such that substrate temperature, working pressure, gas ratio of $Ar/O_{2}$, and rf power density were $640^{\circ}C$, 10 mTorr, 10 seem, and $1.7\;W/cm^{2}$, respectively. In these conditions, the PLT thin film showed the Pb/Ti ratio of 1/2 at the surface, the resistivity of $8{\times}10^{11}{\Omega}{\cdot}cm$, and dielectric constant of 110. The pyroelectric infrared sensors with these PLT thin films showed the peak to peak voltage of 450 m V and signal to noise ratio of 7.2.

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Study on dielectric properties of $Ba_{0.5}Sr_{0.5}TiO_{3}$thin films for high-frequency passive device (고주파 수동소자 유전체용 $Ba_{0.5}Sr_{0.5}TiO_{3}$ 박막의 유전특성에 관한 연구)

  • 이태일;최명률;박인철;김홍배
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2001.07a
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    • pp.263-266
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    • 2001
  • In this paper, we investigated dielectric properies for BST thin films that was deposited on MgO/Si substrates using RF magnetron sputtering. In here, MgO film was used to perform that a diffusion b arrier between the BST film and Si substrate and a buffer layer to assist the BST film growth. A d eposition condition for MgO films was RF Power of 50W, substrate temperature of room temperature and the working gas ratio of Ar:O$_2$ were varied from 90:10 to 60:47. Finally we manufactured the cap acitor of Al/BST/MgO/Si/Al structure to know electrical properties of this capacitor through I-V, C-V measurement. In the results, C-V aha racteristic curves was shown a ferroelectric property so we measured P-E. A remanent poliazation and coerceive electric field was present 2$\mu$C/cm$^2$ and -27kV/cm respectively at Ar:O$_2$=90:10. And a va clue of dielectric constant was 86 at Ar:02=90:10.

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