• Title/Summary/Keyword: CuCa 2at%

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Enhancement of $Bi_2Sr_2Ca_2Cu_3O_{10}$ Formation using $Bi_2Sr_2CuO_6$ and $(Ca_{0.91}Sr_{0.09})CuO_2$ Precursors ($Bi_2Sr_2CuO_6$$(Ca_{0.91}Sr_{0.09})CuO_2$를 이용한 $Bi_2Sr_2Ca_2Cu_3O_{10}$ 고온초전도체의 합성촉진)

  • Lee, Hwa-Sung;Park, Min-Soo;Ahn, Byung-Tae
    • Korean Journal of Materials Research
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    • v.6 no.7
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    • pp.684-691
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    • 1996
  • To enhance the formation of Bi,Sr,Ca,Cu,O,(Bi-2223) single phase in a shorter reaction time, the intermediate compounds such as Bi,Sr,CuO,(Bi-2201). BizSr,CaCuz08(Bi-2212) and (Ca, Sr,, ,9)CuOz in the Bi-Sr-Ca-Cu-0 system were used as the precursors. The formation of Bi-2223 was enhanced in the mixture of Bi-2201 and (Ca, ,,Sr, 119)C~eOsZpe,c ially from the mixture with (Ca, 9I Sr, ,,)CuO,-rich composition compared to Bi, iPb, 4Sr2Ca,Cu3010-cxo mposition. The formation of Bi- 2223 essentially completed within 60h at 860$^{\circ}$C and 870$^{\circ}$C. However, a small amount of the remnant Bi-2212 phase did not disappear even after a prolonged reaction at 870'C. The merit of the proposed synthetic method using the intermediate precusors can be summarized as a shorter reaction time for the formation of Bi-2223 phase, in addition to a smaller amount of second phases compared to the conventional solid-state reaction method.

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luminescent Characteristics of $Ca_{1-x}$Sr$_{x}$S:CuCl Thin-film Electroluminescent(TFEL) Device (Ca$_{1-x}$Sr$_{x}$S:CuCl 박막 전계발광소자의 발광 특성)

  • 이순석;김미혜
    • The Journal of the Korea Contents Association
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    • v.2 no.3
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    • pp.146-151
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    • 2002
  • The $Ca_{1-x}$Sr$_{x}$S:CuCl TFEL devices were fabricated by electron-beam deposition system and luminescent characteristics of the TFEL devices were studied. The SrS and CaS powders were mixed to form $Ca_{1-x}$Sr$_{x}$S host materials and 0.2 at% of CuCl was added as the activator. The luminance(lao) and peak emission wavelength of CaS:CuCl TFEL devices were 9.5 cd/m$^2$ and 492 nm, respectively. The luminance(L$_{30}$) and peak emission wavelength of SrS:CuCl TFEL devices were 633 cd/m$^2$ and 500 nm, respectively. It seems that the addition of CaS into the SrS host material generates blue shift of the EL emission characteristics but reduces the luminance and the luminous efficiency of the $Ca_{1-x}$Sr$_{x}$S:CuCl TFEL devices drastically.

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In doped ZTO 기반 산화물 반도체 TFT 소자의 CuCa 전극 적용에 따른 특성 변화 및 신뢰성 향상

  • Kim, Sin;O, Dong-Ju;Jeong, Jae-Gyeong;Lee, Sang-Ho
    • Proceedings of the Korean Vacuum Society Conference
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    • 2015.08a
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    • pp.167.2-167.2
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    • 2015
  • 고 이동도(~10 cm/Vs), 낮은 공정온도 및 높은 투과율 등의 특성을 갖는 산화물 반도체는 저 소비전력, 대면적화 및 고해상도 LCD Panel에 적합한 재료로서 현재 일부 Mobile Panel 및 TFT-LCD Panel의 양산에 적용되고 있으나, 향후 UHD급(4 K, 8 K)의 대형, 고해상도 Panel에의 적용을 위해서는 30 cm2/Vs 이상의 고 이동도 재료의 개발 및 저 저항 배선의 적용에 따른 소자 신뢰성의 개선이 필요하다. Cu는 대표적인 저 저항 배선 재료로 일부 양산에 적용되고 있으나, Cu 전극과 산화물 반도체의 계면에서 Cu원자의 확산 및 Cu-O 층의 형성에 의한 소자 특성 저하의 문제가 있다. 본 연구에서는 고 이동도의 In doped-ZTO계 산화물 반도체를 기반으로 채널 층과 Cu source-Drain layer의 계면에서의 Cu element의 거동 및 TFT 소자 특성과의 상관관계를 고찰하고, 계면에 형성된 Cu-O layer에 대해 높은 전자 친화도를 갖는 Ca element를 첨가에 의한 TFT 소자 특성의 변화를 관찰하였다. 본 연구에서는 이러한 효과로 인한 소자 신뢰성의 향상을 기대하였으며, 우선 In doped-ZTO 채널 층에 Cu와 CuCa 2at% source-drain을 적용한 TFT 특성을 확인하였다. 그 결과, Cu는 Field-effect mobility: ~17.67 cm2/Vs, Sub-threshold swing: 0.76 mV/decade 및 Vth:, 4.40 V의 결과가 얻어졌으며 CuCa 2at%의 경우 Field-effect mobility: ~17.84 cm2/Vs, Sub-threshold swing: 0.86 mV/decade 및 Vth:, 5.74 V의 결과가 얻어졌다. 소자신뢰성 측면에서도 Bias Stress의 변화량 ${\delta}Vth$의 경우 Cu : 4.48 V에 대해 CuCa 2at% : 2.81 V로 ${\delta}Vth$:1.67 V의 개선된 결과를 얻었다.

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Phase Equilibria for the Formation of Superconducting Phases in the Bi-Sr-Ca-O System (Bi-Sr-Ca-O계에서 초전도상의 형성에 관한 상평형)

  • Kim, Cheol-Jin
    • Korean Journal of Materials Research
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    • v.3 no.4
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    • pp.410-421
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    • 1993
  • Phase equilibria and reaction paths of the superconducting phases and other compatible phases at $850^{\circ}C$ in the Bi-Sr-Ca-Cu-O system were studied. $Bi_2O_3$ was added to $Sr_2CaCu_2O_x$ by 5% up to 40 mole% Bi in the pseudo-binary $Bi_2O_3-(Sr_2CaCu_2O_x)$ system and the heat treated samples were analysed using XRD. SEM, EDS. and DT A. When Bi contents were greater than 35 mole% Bi, liquid phase was formed which was compatible with $Bi_2Sr_2CaCu_2O_8$ phase. The m.p. of $Bi_2Sr_2CaCu_2O_8$ phase decreased as the content of (Sr+Ca)decreased. $Bi_{2+x}Sr_2CaCu_2O_8$ phase first segregated out of liquid phase around $Bi_2Sr_2CaCu_2O_8$ phase during cooling of liquid phase.

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Electrochemical Deposition Characteristics of Ca2+ on Cu Wire Electrode in CaCl2 Molten Salt (CaCl2 용융염에서 Ca2+의 Cu 전극에 대한 전기화학적 증착 특성평가)

  • Hwang, Dong Wook;Lee, Jong Hyeon;Jeong, Sang Mun
    • Korean Chemical Engineering Research
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    • v.60 no.2
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    • pp.175-183
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    • 2022
  • With the expansion of the automobile market, the demand for Nd as an essential rare earth material for automobile motors is rapidly increasing. Research on the calcio-thermic reduction process between Nd2O3 and calcium-based alloys has been extensively studied in order to manufacture Nd. In this study, Ca-Cu, as a reducing for Nd2O3, was prepared by electrolysis in CaCl2 molten salt. Cu wire and graphite were employed as a working electrode and a counter electrode for electrolysis reaction, respectively. The reference electrode was manufactured by putting Ag wire in a mixture of AgCl and CaCl2 at a ratio of 1:99 mol%. The cyclic voltammetry results showed that the deposition of Ca2+ on the surface of working electrode was observed from a potential of -1.8 V, and the reduction potential of Ca2+ decreased as the reaction temperature increased. The diffusion coefficient of Ca2+ calculated by the chronoamperometry experiment was found to be 5.4(±6.8)×10-6 cm2/s. In addition, Ca-Cu liquid alloy was prepared by applying a constant potential to Cu electrodes. The element ratio of Ca-Cu alloy formed by applying a potential of -2.0 V was found to Ca:Cu=1:4.

Optical Characteristics of ZnS/CaF2/ZnS/Cu with Different Optical Thickness of CaF2 Layer (CaF2 두께 변화에 따른 ZnS/CaF2/ZnS/Cu 다층 박막의 광특성)

  • Kim, Jun-Sik;Jang, Gun-Eik
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.22 no.7
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    • pp.584-588
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    • 2009
  • Layered ZnS/$CaF_2$/ZnS/Cu film was deposited on glass substrate by using evaporation method. ZnS and $CaF_2$ were chosen as high and low refractive materials. Cu was used as mid-reflective layer. Reflectance with different optical thickness of $CaF_2$ ranging from $0.25{\lambda}\;to\;0.5{\lambda}$ were systematically investigated by using spectrophotometer. In order to expect the experimental results, the simulation program, the Essential Macleod Program(EMP) was adopted and compared with the experimental data. Based on the results taken by spectrophotometer, the ZnS/$CaF_2$/ZnS/Cu multi-layered thin film show the maximum reflectance of 80% at 625nm $(0.25{\lambda}\;in\;CaF_2)$ and 42% at 660nm $(0.5{\lambda}\;in\;CaF_2)$ respectively. As compared with the experimental results and simulation data, it was confirmed the experimental data is well matched with the EMP data.

Fabrication of $Bi_{2}Sr_{2}CaCu_{2}O_{8}$ Superconducting Films by the LiReac-PreCu Method (급속반응공정에 의한 동 테이프 $Bi_{2}Sr_{2}CaCu_{2}O_{8}$)

  • 성현태;한상철;한영희;이준성;최희락
    • Progress in Superconductivity and Cryogenics
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    • v.1 no.1
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    • pp.7-14
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    • 1999
  • Wekk oriented $Bi_{2} Sr_{2} CaCu_{2} O_{8}$ suppercondcting thick films were fabricared on copper tape by LiReac-PreCu (liquid reaction between a Cu-free precousor and Cu tape) method. Cu-free precursor power which is composed of $Bi_{2}Sr_{2}Ca_{5}$ was printed on a copper tape by screen printing and was heat-treated. The speciment were partially in a molten state at the heat treatment temperature (85$0^{\circ}C$~87$0^{\circ}C$). The heat heat treatments for the reaction were performed in air or low oxygen pressure in several stages. XRD analyses of the resulting Bi2Sr2CaCu2O8 superconducting tapes show that the $Bi_{2} Sr_{2} CaCu_{2} O_{8}$ phase is dominant and a small amount of $Bi_{2} Sr_{2} Cu_{2} O_{6}$ phase is detected. Both phases are aligned in the c-axis direction.

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A Study on Fabrication of $Bi_{2}Sr_{2}Ca_{2}Cu_{3}O_{x}$ Superconductor Thick Films on Cu Substrates (동피복 Bi2223 초전도후막 합성에 관한 연구)

  • 한상철;성태현;한영희;이준성;안재원
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.07a
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    • pp.478-481
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    • 2002
  • We carried out the experiments for fabricating $Bi_{2}Sr_{2}Ca_{2}Cu_{3}O_{x}$(Bi2223) superconductor thick films on Cu tapes. Cu-free (Bi,Pb)-Sr-Ca-0 powder mixtures were screen- printed on Cu tapes and heat-treated at 840-$860^{\circ}C$ for several minutes in air. Surface microstructures and phases of films were analyzed by XRD and optical microscope. The electric properties of superconducting films were examined by the four probe method. At heat-treatment temperature, the printing layers were in a partially molten state by liquid reaction between CuO in the oxidized copper tape and the precursors which were printed on Cu tapes. During the heat-treatment procedure, it is thought that Bi2223 superconducting particles nucleate at interfaces between Bi2212 phase and liquid.

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Float Zone Growth of Superconduction $Bi_2Sr_2CaCu_2O_8$ Fiber with Halogen Lamp (할로겐 램프 열원을 이용한 초전도성 $Bi_2Sr_2CaCu_2O_8$ Fiber의 Float Zone 성장)

  • 김철진;정준기
    • Korean Journal of Crystallography
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    • v.7 no.2
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    • pp.147-155
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    • 1996
  • Floating Zone Image furnace with halogen lamps as heat source has been made and applied to the growth of high-Tc superconductor Bi2Sr2CaCu2O8. The manufactured crystal growth equipment is composed of holder unit for setting the halogen lamps at the focal point of the elliptical mirror, image furnace with maximum temperature of 1800℃ with 1kW halogen lamps, cooling unit, feeding unit for supplying source material to the molten zone, pulling unit for crystal growth, and the control unit in the range of 2mm/hr -40 mm/hr vertical movement and 15rpm - 12rpm rotation. Bi2Sr2CaCu2O8 fibers have been grown with 300W halogen lamps and characterized with XRD, SEM and EDS. The growth condition was air atmosphere, growth speed 3∼4mm/hr, rotation speed of upper and lower part 20∼25 rpm. The fiber was composed of 20∼25 rpm matrix phase and secondary phases such as (Sr,Ca)CuO2 and (Sr,Ca)2CuO3.

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Effect of the Oxygen Partial Pressure on the Phase Stability of ${Bi_2}{Sr_2}{CaCu_2}{O_{8+x}}$ and ${Bi_2}{Sr_2}{Ca_2}{Cu_3}{O_{10+x}}$ (${Bi_2}{Sr_2}{CaCu_2}{O_{8+x}}$${Bi_2}{Sr_2}{Ca_2}{Cu_3}{O_{10+x}}$의 상 안정성에 대한 산소분압의 영향)

  • Park, Min-Su;Lee, Hwa-Seong;An, Byeong-Tae
    • Korean Journal of Materials Research
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    • v.5 no.5
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    • pp.583-597
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    • 1995
  • We investigated the effect of the oxygne partial pressure on the phase stability of B $i_{2}$S $r_{2}$Ca C $u_{2}$ $O_{8+x}$ and B $i_{2}$S $r_{2}$C $a_{2}$C $u_{3}$ $O_{10+x}$ at 82$0^{\circ}C$. As the oxygen pressure decreased, B $i_{2}$Sr/sb 2/CaC $u_{2}$ $O_{8+x}$ melted at 2.2$\times$10$^{-3}$ atm $O_{2}$. In the case of the B $i_{1.7}$P $b_{0.4}$S $r_{2}$C $a_{2}$ $O_{10+x}$, it started to decompose into theree phases of B $i_{2}$S $r_{2}$Cu $O_{6+y}$, $Ca_{2}$Cu $O_{3}$ and C $u_{4}$ $O_{3}$ and C $u_{4}$ $O_{3}$ at 8.0$\times$10$^{-3}$ atm $O_{2}$ and was completely decomposed at 4.3$\times$10$^{-3}$ atm $O_{2}$ B $i_{2}$S $r_{2}$C $a_{2}$C $u_{3}$ $O_{10+x}$ phase was not formed by the solid state reaction from the mixutre of $i_{2}$S $r_{2}$CaCu.sub 2/ $O_{8+x}$, $Ca_{2}$Cu $O_{3}$ and CuO down to 2.2$\times$10.sub -3/ atm O.sub 2/ but formed by the solidifciation of the formed from the mixture of the intermediate compounds in the Bi-Sr-Ca-Cu-O system and the fromation temperature of Bi.sub 2/S $r_{2}$C $a_{2}$Cu.$_{3}$ $O_{10+x}$ can be lowered by reducing oxygen partial pressure.e.e.ure.e.e.

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