• 제목/요약/키워드: $SrTiO_3$ substrate

검색결과 233건 처리시간 0.033초

Noise Properties of Directly-coupled Single-layer High-Tc 2nd-order SQUID Gradiometer

  • 황윤석;안종록;강찬석;이순걸;김진태
    • Progress in Superconductivity
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    • 제3권2호
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    • pp.163-167
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    • 2002
  • We have fabricated planar-type single-layer second-order high-Tc SQUID gradiometers. The devices consisted of symmetrically designed three parallel-connected square pickup loops that were directly coupled to the SQUID. $YBa_2$$Cu_3$$O_{7}$ film was deposited on $SrTiO_3$ substrate by a PLD system and patterned into a device by the photolithography with ion milling technique. Junctions of the SQUID were either step-edge or bicrystal type. All the structures were formed on a 10 mm $\times$ 5 mm substrate. Balancing of the gradiometer was achieved by adjusting the width of the central pickup loop. The gradiometer noise was measured both inside and outside a magnetically shielded room. Details of the results will be discussed.

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SCT 박막의 미세구조 및 구조적인 특성 (Microstructure and Structural Properties of SCT Thin Film)

  • 김진사;오용철
    • 대한전기학회논문지:전기물성ㆍ응용부문C
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    • 제55권12호
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    • pp.576-580
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    • 2006
  • The $(Sr_{0.85}Ca_{0.15})TiO_3(SCT)$ thin films were deposited on Pt-coated electrode $(Pt/TiN/SiO_2/Si)$ using RF sputtering method according to the deposition condition. The crystallinity of SCT thin films were increased with increase of deposition temperature in the temperature range of $100{\sim}500[^{\circ}C]$. The optimum conditions of RF power and $Ar/O_2$ ratio were 140[W] and 80/20, respectively. Deposition rate of SCT thin films was about $18.75[{\AA}/min]$ at the optimum condition. The composition of SCT thin films deposited on Si substrate is close to stoichiometry (1.102 in A/B ratio). The maximum dielectric constant of SCT thin film as obtained by annealing at $600^{\circ}C$.

Growth behavior of YBCO films on STO substrates with ZnO nanorods

  • Oh, Se-Kweon;Lee, Cho-Yeon;Jang, Gun-Eik;Kim, Kyoung-Won;Hyun, Ok-Bae
    • 한국초전도ㆍ저온공학회논문지
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    • 제11권4호
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    • pp.16-19
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    • 2009
  • The influence of nanorods grown on substrate prior to YBCO deposition has been investigated. We studied the microstructures and characteristic of $YBa_2Cu_3O_{7-\delta}$ films fabricated on $SrTiO_3$ (100) substrates with ZnO nanorods as one of the possible pinning centers. The growth density of ZnO nanorods was modulated through Au nanoparticles synthesized on top of the STO(100) substrates with self assembled monolayer. The density of Au nanoparticles is approximately $240{\sim}260\;{\mu}m^{-2}$ with diameters of 41~49 nm. ZnO nanorods were grown on Au nanoparticles by hot-walled PLD with Au nanoparticles. Typical size of ZnO nanorod was around 179 nm in diameter and $2{\sim}6\;{\mu}m$ in length respectively. The ZnO nanorods have apparently randomly aligned and exhibit single-crystal nature along (0002) growth direction. Our preliminary results indicate that YBCO film deposited directly on STO substrate shows the c-axis orientation while YBCO films with ZnO nanorods exhibit any mixed phases without any typical crystal orientation.

SCT 세라믹 박막의 열처리온도 특성 (Properties with Annealing Temperature of SCT Ceramic Thin Film)

  • 김진사;조춘남;오용철;신철기;최운식;김충혁;이준웅
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2002년도 하계학술대회 논문집 Vol.3 No.2
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    • pp.566-569
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    • 2002
  • The $(Sr_{0.9}Ca_{0.1})TiO_3$(SCT) thin films are deposited on Pt-coated electrode (Pt/TiN/$SiO_2$/Si) using RF sputtering method. The maximum dielectric constant of SCT thin film is obtained by annealing at $600[^{\circ}C]$. The temperature properties of the dielectric loss have a value within 0.02 in temperature ranges of $-80{\sim}+90[^{\circ}C]$. The capacitance characteristics had a stable value within ${\pm}4[%]$. The drastic decrease of dielectric constant and increase of dielectric loss in SCT thin films is observed above 200[kHz].

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열처리 온도에 따른 SCT 박막의 미세구조 및 유전특성 (Microstructure and Dielectric Properties of SCT Thin Film with Annealing Temperature)

  • 김진사;조춘남;신철기;박건호;최운식;이성일;이준웅
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 1999년도 추계학술대회 논문집
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    • pp.244-247
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    • 1999
  • The(Sr$\sub$0.85/Ca$\sub$0.15/) TiO$_3$(SCT) thin films are deposited on Pt-coated electrode(Pt/TiN/SiO$_2$/Si) using RF sputtering method. The composition of SCT thin films deposited on Si substrate at room temperature is close to stoichiometry(1.102 in A/B ratio). Also, SCT thin films deposited on Pt-coated electrodes have the cubic perovskite structure and polycrystalline state. The maximum dielectric constant of SCT thin films is obtained by annealing at 600[$^{\circ}C$].The dielectric constant changes almost linearly in temperature ranges of -80~+90[$^{\circ}C$].

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HIGH TEMPERATURE SUPERCONDUCTING THIN FILMS PREP ARED BY PULSED LASER DEPOSITION

  • Park, Yong-Ki;Kim, In-Seon;Ha, Dong-Han;Hwang, Doo-Sup;Huh, Yun-Sung;Park, Jong-Chul
    • 한국표면공학회지
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    • 제29권5호
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    • pp.430-436
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    • 1996
  • We have grown superconducting thin films on various substrates using a pulsed laser deposition (PLD) method. $YBa_2Cu_3O_7-\delta$ (YBCO) superconducting thin films with the superconducting transition temperature ($T_{c. offset}$) of 87K were grown on Si substrates using yittria-stabilized zirconia (YSZ) and $CeO_2$ double buffer layers. We have developed a large area pulsed laser deposition system. The system was designed to deposit up to 6 different materials on a large area substrate up to 7.5cm in diameter without breaking a vacuum. The preliminary runs of the deposition of YBCO superconducting thin films on $SrTiO_3$ substrate using this system showed a very uniform thickness profile over the entire substrate holder area. $T_{c}$ of the deposited YBCO thin film, however, was scattered depending on the position and the highest value was 85K.

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Multi-coated YBa2Cu3O7-x Films Fabricated by a Fluorine-Free Sol-Gel Process

  • Cho, E.A.;Jang, G.E.;Hyun, O.B.
    • Journal of Magnetics
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    • 제16권2호
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    • pp.186-191
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    • 2011
  • [ $YBa_2C_3O_{7-x}$ ]films were fabricated on a $SrTiO_3$ (100) substrate using a trimethylaceate propionic acid (TMAP)-based MOD process by controlling the precursor solution viscosity, firing temperature, and by using various coatings. The viscosity of the precursor solution was controlled by the addition of Xylenes. The films were heat treated with different temperatures from 750 to $800^{\circ}C$. c-axis oriented films were obtained. After adding 9 ml of Xylene into the precursor solution, the $T_c$ of the YBCO film, which was coated 2 times and heat treated at $800^{\circ}C$, was 86 K and the measured $J_c$ was above 2.5 MA/$cm^2$ at 77 K in a zero-field.

MOCVD 법에 의해 제조된 $CeO_2$ 버퍼층 증착 거동의 기판 의존성 (Substrate dependence of the deposition behavior of $CeO_2$ buffer layer prepared by MOCVD method)

  • 전병혁;최준규;정우영;이희균;홍계원;김찬중
    • Progress in Superconductivity
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    • 제7권2호
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    • pp.130-134
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    • 2006
  • Buffer layers such as $CeO_2\;and\;Yb_2O_3$ films for YBCO coated conductors were deposited on (100) $SrTiO_3$ single crystals and (100) textured Ni substrates by a metal organic chemical vapor deposition (MOCVD) system of the hot-wall type. The substrates were moved with the velocity of 40 cm/hr. Source flow rate, $Ar/O_2$ flow rate and deposition temperature were main processing variables. The degree of film epitaxy and surface morphology were investigated using XRD and SEM, respectively. On a STO substrate, the $CeO_2$ film was well grown epitaxially above the deposition temperature of $450^{\circ}C$. However, on a Ni substrate, the XRD showed NiO (111) and (200) peaks due to Ni oxidation as well as (111) and (200) film growth. For the films deposited with $O_2$ gas as oxygen source, it was found that the NiO film was formed at the interface between the buffer layer and the Ni substrate. The NiO layer interrupts the epitaxial growth of the buffer layer. It seems that the epitaxial growth of the buffer layer on Ni metal substrates using $O_2$ gas is difficult. We are considering a new method avoiding Ni oxidation with $H_2O$ vapor instead of $O_2$ gas.

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열처리에 따른 Pb[(Zr,Sn)Ti]N$bO_3$ 박막의 강유전 특성 (Ferroelectric Properties of Pb[(Zr,Sn)Ti]N$bO_3$ Thin Films by Annealing)

  • 최우창;최혁환;이명교;권태하
    • 대한전자공학회논문지SD
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    • 제38권7호
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    • pp.473-478
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    • 2001
  • 강유전 물질인 Pb/sub 0.99/[(Zr/sub 0/6Sn/sub 0.4/)/0.9/Ti/sub 0.1/]0.98/Nb/sub 0.02/O₃(PNZST) 박막을 10 mole%의 과잉 PbO가 첨가된 타겟을 이용하여 La/sub 0.5/Sr/sub 0.5/CoO₃(LSCO)/Pt/Ti/SiO₂/Si 기판상에 RF 마그네트론 스퍼터링 방법으로 증착하였다. 증착된 박막에 대하여 온도와 시간을 다양하게 변화시키면서 급속 열처리(rapid thermal annealing) 한 후, 그 결정성과 전기적 특성을 조사하였다. 80 W의 RF 전력, 500 ℃의 기판온도에서 증착한 후, 급속 열처리된 박막이 페로브스카이트상으로 결정화되었으며, 650 ℃, 공기중에서 10초동안 급속 열처리된 박막이 가장 우수한 결정성을 나타내었다. 이러한 박막으로 제작된 PNZST 커패시터는 약 20 μC/㎠정도의 잔류 분극과 약 50 kV/cm 정도의 항전계를 나타내었으며, 2.2×10/sup 9/의 스위칭 후에도 잔류분극의 감소는 10 %미만이었다.

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메모리 소자에의 응용을 위한 SrBi2Nb2O9 박막의 성장 및 전기적 특성 (Growth and Characteristics of SrBi2Nb2O9 Thin Films for Memory Devices)

  • 강동훈;최훈상;이종한;임근식;장유민;최인훈
    • 한국재료학회지
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    • 제12권6호
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    • pp.464-469
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    • 2002
  • $SrBi_2Nb_2O_9(SBN)$ thin films were grown on Pt/Ti/Si and p-type Si(100) substrates by rf-magnetron co-sputtering method using two ceramic targets, $SrNb_2O_6\; and \;Bi_2O_3$. The structural and electrical characteristics have been investigated to confirm the possibility of the SBN thin films for the applications to destructive and nondestructive read out ferroelectric random access memory(FRAM). For the optimum growth condition X-ray diffraction patterns showed that SBN films had well crystallized Bi-layered perovskite structure after $700^{\circ}C$ heat-treatment in furnace. From this specimen we got remnant polarization $(2P_r)$ of about 6 uC/$\textrm{cm}^2$ and coercive voltage $(V_c)$ of about 1.5 V at an applied voltage of 5 V. The leakage current density was $7.6{\times}10^{-7}$/A/$\textrm{cm}^2$ at an applied voltage of 5V. And for the NDRO-FRAM application, properties of SBN films on Si substrate has been investigated. From transmission electron microscopy (TEM) analysis, we found the furnace treated sample had a native oxide about 2 times thicker than the RTA treated sample and this thick native oxide layer had a bad effect on C-V characteristics of SBN/Si thin film. After $650^{\circ}C$ RTA process, we got the improved memory window of 1.3 V at an applied voltage of 5 V.