• 제목/요약/키워드: Deposition Process

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New Selective Tungsten Deposition Process by the alternating Cyclic Hydrogen Reduction of $WF_6$ using LPCVD (LPCVD을 사용하여 $WF_6$의 교번적 수소환원 반응에 의한 새로운 선택적 텅스텐 박막 증착)

  • ;Arnold Reisman;Christopher Berry
    • The Transactions of the Korean Institute of Electrical Engineers
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    • v.39 no.7
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    • pp.692-701
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    • 1990
  • New selective tungsyen deposition deposition on silicon process is described which makes use of a previously unreported, alternating cyclic,

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Fabrication of YSZ-based Micro Tubular SOFC Single Cell using Electrophoretic Deposition Process

  • Yu, Seung-Min;Lee, Ki-Tae
    • Journal of the Korean Ceramic Society
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    • v.52 no.5
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    • pp.315-319
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    • 2015
  • Yttria-stabilized zirconia (YSZ)-based micro tubular SOFC single cells were fabricated by electrophoretic deposition (EPD) process. Stable slurries for the EPD process were prepared by adding phosphate ester (PE) as a dispersant in order to control the pH, conductivity, and zeta-potential. NiO-YSZ anode support, NiO-YSZ anode functional layer (AFL), and YSZ electrolyte were consecutively deposited on a graphite rod using the EPD process; materials were then co-sintered at $1400^{\circ}C$ for 4 h. The thickness of the deposited layer increased with increasing of the applied voltage and the deposition time. A YSZ-based micro tubular single cell fabricated by the EPD process exhibited a maximum power density of $0.3W/cm^2$ at $750^{\circ}C$.

Particle Deposition, PD Process - New Potential in Material Processing -

  • Fukumoto, Masahiro
    • Proceedings of the Korean Powder Metallurgy Institute Conference
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    • 2006.09a
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    • pp.47-48
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    • 2006
  • Oridinal thermal spray process has developed into two ways, namely, temperature dominated represented by plasma spraying, and velocity dominated represented by HVOF. It is common for both that the particle materials sprayed are basically in melted or half melted condition. New process has developed recently, that is, Cold Spray and Aerosol Deposition. Particle's heating is limited in CS lower than half of the material's melting point. Moreover, exactly no heating is loaded in AD process. Through the investigation on common feature for these three spraying processes, potential of new material process - Particle Deposition, PD - is considered and proposed.

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HIGH-THROUGHPUT PROCESS FOR ATOMIC LAYER DEPOSITION

  • Shin, Woong-Chul;Choi, Kyu-Jeong;Baek, Min;Kim, Mi-Ry
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2009.11a
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    • pp.23.2-23.2
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    • 2009
  • Atomic layer deposition (ALD)have been proven to be a very attractive technique for the fabrication of advanced gate dielectrics and DRAM insulators due to excellent conformality and precise control of film thickness and composition, However, one major disadvantages of ALD is its relatively low deposition rate (throughput) because the deposition rate is typically limited by the time required for purging process between the introduction of precursors. In order to improve its throughput, many efforts have been made by commercial companies, for example,the modification reactor and development of precursors. However, any promising solution has not reported to date. We developed a new concept ALD system(Lucida TM S200) with high-throughput. In this process, a continuous flow of ALD precursor and purging gas are simultaneously introduced from different locations in the ALD reactor. A cyclic ALD process is carried out by moving the wafer holder up and down. Therefore, the time required for ALD reaction cycle is determined by speed of the wafer holder and vapor pressure of precursors. We will present the operating principle of our system and results of deposition.

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Silicon Carbide Coating by Thermal Decomposition of tetramethylsilane

  • YOON Kyung-Hoon
    • Proceedings of the Korean Ceranic Society Conference
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    • 1986.12a
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    • pp.211-225
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    • 1986
  • Silicon carbide coating has been studied using a graphite substrate, a mixture of tetramethylsilane and hydrogen or argon at deposition temperature (T) of 950 to $1200^{\circ}C$ total pressure of 20 to 50 torr and carrier gas flow rate of 0 to 901/h. Deposition kinetic study has shown that a transition, from a surface reaction limited process to a diffusion limited one, takes place near $1100^{\circ}C$. Deposition rate depends directly upon the experimental parameters. The influence of the main process parameters is also discussed to relate the physiochemical properties of the coating to the deposition conditions.

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A Thermodynamic Analysis on Silicon Consumption during The Chemical Vapper Deposition of Tungsten (텅스텐의 화학증착시 Si소모에 관한 열역학적 분석)

  • 정태희;이정중
    • Journal of the Korean institute of surface engineering
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    • v.23 no.1
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    • pp.27-33
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    • 1990
  • Thermodynamic analysis on silicon consumpton during the chemical vapor deposition of tungten was carried out by calculation equilibrium concerations of all possible product species utilizing a computer progrom according to VCS.(Villars-Cruise-Smith) algorithm. The calculation could show various reaction paths which dominate the tungsten deposition under different process conditions. According to the calculation, the consumption of silicon can also be reduced at a lower total pressure SiH4 without H2 as the reacting gas is most effective for suppression of the excessive consumption of silicon during the deposition process.

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The ZnS Film Deposition Technology for Cd-free Buffer Layer in CIGS Solar Cells

  • Lee, Jae-Hee;Hwang, Do-Weon
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.08a
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    • pp.218-218
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    • 2011
  • The CIGS Solar Cells have the highest conversion efficiency in the film-type solar cells. They consist of p-type CuInSe2 film and n-type ZnO film. The CdS films are used as buffer layer in the CIGS solar cells since remarkable difference in the lattice constant and energy band gap of two films. The CdS films are toxic and make harmful circumstances. The CdS films deposition process need wet process. In this works, we design and make the hitter and lamp reflection part in the sputtering system for the ZnS films deposition as buffer layer, not using wet process. Film thickness, SEM, and AFM are measured for the uniformity valuation of the ZnS films. We conclude the optimum deposition temperature for the films uniformity less than 1.6%. The ZnS films deposited by the sputtering system are more dense and uniform than the CdS films deposited by the Chemical Bath Deposition Method(CBD) for the CIGS Solar Cells.

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XRD Patterns and Bismuth Sticking Coefficient in $Bi_2Sr_2Ca_nCu_{n+1}O_y(n\geq0)$ Thin Films Fabricated by Ion Beam Sputtering Method

  • Yang, Seung-Ho;Park, Yong-Pil
    • Journal of information and communication convergence engineering
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    • v.4 no.4
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    • pp.158-161
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    • 2006
  • [ $Bi_2Sr_2Ca_nCu_{n+1}O_y(n{\geq}0)$ ] thin film is fabricatedvia two different processes using an ion beam sputtering method i.e. co-deposition and layer-by-layer deposition. A single phase of Bi2212 can be fabricated via the co-deposition process. While it cannot be obtained by the layer-by-layer process. Ultra-low growth rate in our ion beam sputtering system brings out the difference in Bi element adsorption between the two processes and results in only 30% adsorption against total incident Bi amount by layer-by-layer deposition, in contrast to enough Bi adsorption by co-deposition.

Effect of Torch Speed and Solid Layer Thickness on Heat Transfer and Particle Deposition During modified Chemical Vapor Deposition Process (수정된 화학증착과정에서 토치이송과 고체층이 열전달과 입자부착에 미치는 영향)

  • 박경순;최만수
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.18 no.5
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    • pp.1301-1309
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    • 1994
  • A study of heat transfer and thermophoretic particle deposition has been carried out for the Modified Chemical Vapor Deposition(MCVD) process. A new concept utilizing two torches is suggested to simulate the heating effects from repeated traversing torches. Calculation results for the wall temperatures and deposition efficiency are in good agreement with experimental data. The effects of variable properties are included and heat flux boundary condition is used to simulate the moving torch heating. A conjugate heat transfer which includes heat conduction through solid layer and heat teansfer in a gas in a tube is analyzed. Of particular interests are the effects of torch speeds and solid layer thicknesses on the deposition efficiency, rate and the tapered entry length.