• Title/Summary/Keyword: Deposition temperature

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Preparation of ATO Thin Films by DC Magnetron Sputtering (I) Deposition Characteristics (DC Magnetron Sputtering에 의한 ATO 박막의 제조 (I)증착특성)

  • Yoon, C.;Lee, H.Y.;Chung, Y.J.
    • Journal of the Korean Ceramic Society
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    • v.33 no.4
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    • pp.441-447
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    • 1996
  • Sb doped SnO2(ATO:Antinomy doped Tin Oxide) thin films were prepared by a DC magnetron spttuering method using oxide target and the deposition characteristics were investigated. The experimental conditions are as follows :Ar flow rate : 100 sccm oxygen flow rates ; 0-100 sccm deposition temperature ; 250 -40$0^{\circ}C$ DC sputter powder ; 150~550 W and sputtering pressure ; ; 2~7 mTorr. Deposition rate greatly depends not on the deposition temperature but on the reaction pressure oxygen flow rate and sputter power,. when the sputter powder is low ATO thin films with (110) preferred orientation are deposited. And when the sputter power is high (110) prefered orientation appeares with decreasing of oxygen flow rate and increasing of suputte-ring pressure.

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Deposition of Epitaxial Silicon by Hot-Wall Chemical Vapor Deposition (CVD) Technique and its Thermodynamic Analysis

  • Koh, Wookhyun;Yoon, Deoksun;Pa, ChinHo
    • Proceedings of the Korea Association of Crystal Growth Conference
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    • 1998.06a
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    • pp.173-176
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    • 1998
  • Epitaxial Si layers were deposited on n- or p-type Si(100) substrates by hot-wall chemical vapor deposition (CVD) technique using the {{{{ {SiH }_{ 2} {Cl }_{2 } - {H }_{ 2} }}}}chemistry. Thermodynamic calculations if the Si-H-Cl system were carried out to predict the window of actual Si deposition procedd and to investigate the effects of process variables(i.e., the deposition temperature, the reactor pressure, and the source gas molar ratios) on the growth of epitaxial layers. The calculated optimum process conditions were applied to the actual growth runs, and the results were in good agreement with the calculation. The expermentally determined optimum process conditions were found to be the deposition temperature between 900 and 9$25^{\circ}C$, the reactor pressure between 2 and 5 Torr, and source gad molar ration({{{{ {H }_{2 }/ {SiH }_{ 2} {Cl }_{2 } }}}}) between 30 and 70, achieving high-quality epitaxial layers.

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A Study on the Pulsed Laser Deposition of Diamond like Carbon Thin Films (다이아몬드상 카본박막의 펄스레이저 증착법 연구)

  • Sim, Gyeong-Seok;Lee, Sang-Ryeol
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.48 no.6
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    • pp.403-409
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    • 1999
  • We fabricated diamond like carbon (DLC) thin films using pulsed laser deposition (PLD) method. Among many deposition parameters, the effects of the deposition temperature and the laser energy density were investigated. Structural properties of the films were studied by Raman spectroscopy. The surface morphologies and cross-section imagies of the films were investigated by atomic force microscopy (AFM) and scanning electron microscopy (SEM) respctively. DLC thin films fabricated at $12 J/cm^2$ of a laser energy density and $300^{\circ}C$ of a deposition temperature showed the best quality.

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Studies on Film Growth and Mechanical Properties of TiN by Chemical Vapor Deposition (화학증착에 의한 TiN 박막의 제조 및 기계적 성질에 관한 연구)

  • 김시범;김광호;천성순
    • Journal of the Korean Ceramic Society
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    • v.26 no.1
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    • pp.21-30
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    • 1989
  • Titanium Nitride (TiN) was deposited onto the SKH9 tool steels by chemical vapor deposition (CVD) using a gaseous mixture of TiCl4, N2, and H2. The effects of the deposition temperature and input gas composition on the deposition rate, microstructure, preferred orientation, microhardness and wear resistance of TiN deposits were studied. The experimental results showed that the TiN deposition is thermally activated process with an apparent activation energy of about 27Kcal/mole in the temperature range between 1200$^{\circ}$K and 1400$^{\circ}$K. As H2/N2 gas input ratio increased, the deposition rate increased, showed maximum at H2/N2 gas input ratio of 1.5 and then decreased. Mechanical properties such as microhardness and wear resistance have close relation with the microstructure and preferred orientation of TiN deposits. It is suggested that the equiaxed structure with random orientation increases the microhardness and wear resistance of TiN deposits.

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A Nano-particle Deposition System for Ceramic and Metal Coating at Room Temperature and Low Vacuum Conditions

  • Chun, Doo-Man;Kim, Min-Hyeng;Lee, Jae-Chul;Ahn, Sung-Hoon
    • International Journal of Precision Engineering and Manufacturing
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    • v.9 no.1
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    • pp.51-53
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    • 2008
  • A new nano-particle deposition system (NPDS) was developed for a ceramic and metal coating process. Nano- and micro-sized powders were sprayed through a supersonic nozzle at room temperature and low vacuum conditions to create ceramic and metal thin films on metal and polymer substrates without thermal damage. Ceramic titanium dioxide ($TiO_2$) powder was deposited on polyethylene terephthalate substrates and metal tin (Sn) powder was deposited on SUS substrates. Deposition images were obtained and the resulting chemical composition was measured using X-ray photoelectron spectroscopy. The test results demonstrated that the new NPDS provides a noble coating method for ceramic and metal materials.

Construction of CVD by using RF Helicon Plasma (RF 헬리콘 플라즈마를 이용한 회학기상 증착기의 제작)

  • 신재균;현준원;박상규
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.11 no.8
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    • pp.607-612
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    • 1998
  • RF HPCVD(Helicon Plasma Chemical Vapor Deposition) has been successfully constructed for diamond thin films. The system consists of plasma generation tube, deposition chamber, pumping lines for gas system. A mixture of $CH_4 and H_2$is used for reaction. Two thermocouples, a quartz tube surrounded by a RF antenna and a magnet, and a high temperature heater were set up in the deposition chamber. The process for the thin film diamond deposition has been carried put in a high vacuum system at a substrate temperature of $800^{\circ}C$, and pressure of 5 mtorr. It is also demonstrated. that the RF HPCVD system has advantages for controlling deposition parameters easily.

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Effects of Inner Jet Injection on Particle Deposition in the Annular Modified Chemical Vapor Deposition Process Using Concentric Tubes (환상형원관을 사용하는 수정된 화학증착(MCVD)방법에서 내부 제트분사가 입자부착에 미치는 영향)

  • 최만수;박경순
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.18 no.1
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    • pp.212-222
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    • 1994
  • In the annular Modified Chemical Vapor Deposition process using two concentric tubes, the inner tube is heated to maintain high temperature gradients to have high thermophoretic force which can increase particle deposition efficiency. However, higher axial velocity in a narrow gap between inner and outer tubes can result in a longer tapered entry length. In the present paper, a new concept using an annular jet from the inner tube is presented and shown to significantly reduce the tapered entry length with maintaining high efficiency. Effects of a jet injection on heat transfer, fluid flow and particle deposition have been studied. Of particular interests are the effects of jet velocity, jet location and temperature on the deposition efficiency and tapered length . Torch heating effects from both the previous and present passes are included and the effect of surface radiation between inner and outer tubes is also considered.

Surface Modification Using CVD-SiC (화학증착 탄화규소에 의한 표면 개질)

  • 김한수;최두진;김동주
    • Journal of the Korean Ceramic Society
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    • v.33 no.7
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    • pp.761-770
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    • 1996
  • Silicon carbide (SiC) films were deposited by low pressure chemical vapor deposition (LPCVD) using MTS (CH3SICl3) in a hydrogen atmosphere onto graphite substrates. Depletion effects of reactants which usually occur in the hot wall horizaontal reactor were increased with deposition temperature and pressure. Below 50 torr of total pressure (111) plane was preferenctially grown irrespectrive of deposition temperature and deposition site. Over 50 torr of total pressure however (220) plane was preferentially deposited under 130$0^{\circ}C$ and at inlet site. The surface morphologies of SiC films were uniform at all deposition sites under low pressure but greatly changed with pressure. It shows that a facet structure which was formed above 125$0^{\circ}C$ played an important role in the changed of preferred orientation and surface roughness.

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Studies on Electroless Nickel Plating on Alumina Ceramics(I) on Empirical Deposition Rate in Electroless Nickel Plating (알루미나 세라믹스 표면에 무전해 환원 니켈막의 형성에 관한 연구(I) 무전해 니켈도금의 실험적 석출속도에 관한 연구)

  • Kim, Yong-Dai;Lee, Joon
    • Journal of the Korean institute of surface engineering
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    • v.19 no.3
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    • pp.109-120
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    • 1986
  • The electroless nickel plating on high alumina ceramics was performed in the bath containing nickel chloride, sodium hypophosphite and mono- or bi-carboxylic acid as a complexing agent in order to examine the empirical rate law as well as the effects of the complexing agent, plating temperature and pH on the rate of deposition. Adding the carboxylic acid to the plating bath, the rate of deposition was increased considerably, and each of the complexing agents showed a maximum deposition rate plateau around a particular concentration of the complexing agent. The rate of deposition was increased with increasing either temperature or pH, but microstructure of the surface became more rough. Furthermore, empirical rate law of the elecltroless nickel deposition on high alumina ceramics was discussed with the activation energy and other rate parameters calculated.

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Pyrolytic Carbon Coating on A Simulated Fuel by Fluidized Bed Type Chemical Vapour Deposition

  • Park, Y.;Kim, Bong G.;Lee, Young W.;Dong S. Sohn
    • Proceedings of the Korean Nuclear Society Conference
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    • 1997.05b
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    • pp.159-164
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    • 1997
  • Pyrolytic carbon layer was coated on A1203 balls by fluidized bed type chemical vapour deposition unit to develop the coating technology for the preparation of coated nuclear fuel. The deposition was carried out at the temperature ranges between 110$0^{\circ}C$ and 130$0^{\circ}C$ with various gas contents and flow rates. Source and carrier gas were propane and argon, respectively. X-ray analysis shows that the deposition layer was typical carbon spectra. The growth rate of carbon layer depended on the amount of source gas and the deposition temperature. For the alumina balls with 2mm in diameter, the deposition rate was 11${\mu}{\textrm}{m}$/hr in the flow gases containing 30% source gas at 130$0^{\circ}C$ with a total flow rate of 2.0$\ell$/min. Microstructural observation of the deposits with scanning electron microscope revealed that the deposits had relatively dense and isotropic structure. Chemical analysis by energy dispersive spectroscopy showed that the layer was pure carbon.

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