• Title/Summary/Keyword: Deposition chamber

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Analysis of New DI Diesel Combustion Chamber System using New Spray Wall Impaction Model (새로운 충돌모델을 이용한 신형식 디젤연소실 분석)

  • Chang W. S.;Kim D. J.;Park K.
    • Journal of computational fluids engineering
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    • v.2 no.1
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    • pp.54-65
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    • 1997
  • Wall wetting in diesel engines has been considered as a bad phenomenon because of fuel deposition which makes fuel/air mixing and evaporation worse. In order to avoid the problem, many research works have been carried out. One of the studies is on new combustion chamber systems which are using spray impacting on a wall. In this study a new type of chamber system is analysed using wall impaction model introduced and assessed in the coupled paper. The gas phase is modelled in terms of the Eulerian continuum conservation equations of mass, momentum, energy and fuel vapour fraction, The liquid phase is modelled following the discrete droplet model approach in Lagrangian form. With various conditions the spray distribution, vapor contour and gas flows are analyzed, and then design factors of those combustion systems are recommended.

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Study for Gas Flow Uniformity Through Changing of Shape At the High Density Plasma CVD (HDP CVD) Chamber (HDP CVD 챔버 형상 변화에 따른 가스 유동 균일성에 대한 연구)

  • Jang, Kyung-Min;Kim, Jin-Tae;Hong, Soon-Il;Kim, Kwang-Sun
    • Journal of the Semiconductor & Display Technology
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    • v.9 no.4
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    • pp.39-43
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    • 2010
  • According to recent changes in industry for the semiconductor device, a gap between patterns in wafer is getting narrow. And this narrow gap makes a failure of uniform deposition between center and edge on the wafer. In this paper, for solving this problem, we analyze and manipulate the gas flow inside of the HDP CVD chamber by using CFD(Computational Fluid Dynamics). This simulation includes design manipulations in heights of the chamber and shape of center nozzle in the upper side of the chamber. The result of simulation shows 1.28 uniformity which is lower 3% than original uniformity.

Design and construction of a new ultraviolet sensor using CsI deposition in the ionization chamber

  • Souri, R.;Negarestani, A.;Souri, S.;Farzan, M.;Mahani, M.
    • Nuclear Engineering and Technology
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    • v.50 no.5
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    • pp.751-757
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    • 2018
  • In this article, a UV sensor that is an appropriate tool for fire detection has been designed and constructed. The structure of this UV sensor is an air-filled single-wire detector that is able to operate under normal air condition. A reflective CsI photocathode is installed at the end of the sensor chamber to generate photoelectrons in the ion chamber. An electric current is produced by accelerating photoelectrons to the anode in the electric field. The detector is able to measure the intensity of the incident UV rays whenever the current is sufficiently high. Therefore, the sensitivity coefficient of this sensor is found to be $7.67{\times}10^{-6}V/photons/sec$.

High-Efficiency a-Si:H Solar Cell Using In-Situ Plasma Treatment

  • Han, Seung Hee;Moon, Sun-Woo;Kim, Kyunghun;Kim, Sung Min;Jang, Jinhyeok;Lee, Seungmin;Kim, Jungsu
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.02a
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    • pp.230-230
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    • 2013
  • In amorphous or microcrystalline thin-film silicon solar cells, p-i-n structure is used instead of p/n junction structure as in wafer-based Si solar cells. Hence, these p-i-n structured solar cells inevitably consist of many interfaces and the cell efficiency critically depends on the effective control of these interfaces. In this study, in-situ plasma treatment process of the interfaces was developed to improve the efficiency of a-Si:H solar cell. The p-i-n cell was deposited using a single-chamber VHF-PECVD system, which was driven by a pulsed-RF generator at 80 MHz. In order to solve the cross-contamination problem of p-i layer, high RF power was applied without supplying SiH4 gas after p-layer deposition, which effectively cleaned B contamination inside chamber wall from p-layer deposition. In addition to the p-i interface control, various interface control techniques such as thin layer of TiO2 deposition to prevent H2 plasma reduction of FTO layer, multiple applications of thin i-layer deposition and H2 plasma treatment, H2 plasma treatment of i-layer prior to n-layer deposition, etc. were developed. In order to reduce the reflection at the air-glass interface, anti-reflective SiO2 coating was also adopted. The initial solar cell efficiency over 11% could be achieved for test cell area of 0.2 $cm^2$.

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In Situ X-ray Photoemission Spectroscopy Study of Atomic Layer Deposition of $TiO_2$ on Silicon Substrate

  • Lee, Seung-Youb;Jeon, Cheol-ho;Kim, Yoo-Seok;Kim, Seok-Hwan;An, Ki-Seok;Park, Chong-Yun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.08a
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    • pp.222-222
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    • 2011
  • Titanium dioxide (TiO2) has a number of applications in optics and electronics due to its superior properties, such as physical and chemical stability, high refractive index, good transmission in vis and NIR regions, and high dielectric constant. Atomic layer deposition (ALD), also called atomic layer epitaxy, can be regarded as a special modification of the chemical vapor deposition method. ALD is a pulsed method in which the reactant vapors are alternately supplied onto the substrate. During each pulse, the precursors chemisorb or react with the surface groups. When the process conditions are suitably chosen, the film growth proceeds by alternate saturative surface reactions and is thus self-limiting. This makes it possible to cover even complex shaped objects with a uniform film. It is also possible to control the film thickness accurately simply by controlling the number of pulsing cycles repeated. We have investigated the ALD of TiO2 at 100$^{\circ}C$ using precursors titanium tetra-isopropoxide (TTIP) and H2O on -O, -OH terminated Si surface by in situ X-ray photoemission spectroscopy. ALD reactions with TTIP were performed on the H2O-dosed Si substrate at 100$^{\circ}C$, where one cycle was completed. The number of ALD cycles was increased by repeated deposition of H2O and TTIP at 100$^{\circ}C$. After precursor exposure, the samples were transferred under vacuum from the reaction chamber to the UHV chamber at room temperature for in situ XPS analysis. The XPS instrument included a hemispherical analyzer (ALPHA 110) and a monochromatic X-ray source generated by exciting Al K${\alpha}$ radiation (h${\nu}$=1486.6 eV).

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Development of the Novel Dry and Wet Deposition Collector (새로운 건성 및 습성 침착 채취기의 개발)

  • 이병규;이채복
    • Journal of Korean Society for Atmospheric Environment
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    • v.16 no.6
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    • pp.675-684
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    • 2000
  • A novel dry and wet deposition collector, which can overcome the several problems such as water evaporation cartridge cracks and high costs founded in the previous collector systems, has been constructed. ENVI-18 SPE adsorption cartridge has been used to measure atmospheric deposition of polycylic aromatic hydrocarbons (PAHs). A surrogate surface, consisted of water and methanol, was filled in the dry deposition funnel to simulate dry deposition onto water surface. A water supply system in order to compensat evaporation of the surrogate surface was used and it was consisted of a piston pump, a tubing pump, a overflow tube and a chamber system. A novel water vaporizing system to supply water onto the wet SPE cartridge system with a constant flow rate was developed. The novel water vaporizing system, consisted of a vacuum pump, a water supply reserviour and tube and a mini space heater, could prevent the PAHs adsorption cartridge cracks occurred in the previous collector and effectively adsorb PAHs. The novel dry and wet deposition collector showed a good adsorption, desorption, and recovery rates of PAHs. By reducing the number of pumps used and employing polypyopylene (PP) instead of teflon as a material of collection funnel, the total construction costs were much reduced as compared with the previous dry and wet deposition collectors.

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Simulation and Characteristic Measurement with Sputtering Conditions of Triode Magnetron Sputter

  • Kim, Hyun-Hoo;Lim, Kee-Joe
    • Transactions on Electrical and Electronic Materials
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    • v.5 no.1
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    • pp.11-14
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    • 2004
  • An rf triode magnetron sputtering system is designed and installed its construction in vacuum chamber. In order to calibrate the rf triode magnetron sputtering for thin films deposition processes, the effects of different glow discharge conditions were investigated in terms of the deposition rate measurements. The basic parameters for calibrating experiment in this sputtering system are rf power input, gas pressure, plasma current, and target-to-substrate distance. Because a knowledge of the deposition rate is necessary to control film thickness and to evaluate optimal conditions which are an important consideration in preparing better thin films, the deposition rates of copper as a testing material under the various sputtering conditions are investigated. Furthermore, a triode sputtering system designed in our team is simulated by the SIMION program. As a result, it is sure that the simulation of electron trajectories in the sputtering system is confined directly above the target surface by the force of E${\times}$B field. Finally, some teats with the above 4 different sputtering conditions demonstrate that the deposition rate of rf triode magnetron sputtering is relatively higher than that of the conventional sputtering system. This means that the higher deposition rate is probably caused by a high ion density in the triode and magnetron system. The erosion area of target surface bombarded by Ar ion is sputtered widely on the whole target except on both magnet sides. Therefore, the designed rf triode magnetron sputtering is a powerful deposition system.

The Physical Properties of Silicon and Silicon-Oxide by Epitaxial Growth (1) (기상성장에 의한 Si단결정과 Si산화막의 특성( 1 ))

  • 성영권;오석주;김석기;이상수
    • 전기의세계
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    • v.22 no.2
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    • pp.11-18
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    • 1973
  • This paper reports some results of Si and SiO$_{2}$ films obtained from the expitaxial growth by hydrogen reduction of SiCI$_{4}$ with a hydrogen and carbon dioxide mixture in an epitaxial-deposition chamber. The deposited Si and SiO$_{2}$ are studied by observing the process parameters affecting the rate of deposition, and the quantitative properties at the interface of Si and SiO$_{2}$ are also considered briefly according to the results of the optical absorption and the voltage-current characteristic of MOS etc. using step etching procedure for oxide films.

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Design of equipment for multi-layer sputtering deposition (다층막 스퍼터링 증착장치의 설계)

  • Kim, Soo-Yong;Jung, Won-Chae
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.11a
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    • pp.548-550
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    • 2002
  • 본 장치는 다층막 스퍼터링 증착장치로써 박막을 증착시키는데 용이하게 설계하는 것이 목적이며, 박막두께가 균일하게 증착되고 진공조 내부의 압력을 일정하게 제어가 가능하고 배기시스템은 스퍼터실과 증착실의 진공배기를 공용으로 구조를 설계하여 장치의 스퍼터링 증착조건에 적합하도록 연구실험용으로 설계되어졌다.

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Particle deposition on a semiconductor wafer larger than 100 mm with electrostatic effect (정전효과가 있는 100mm보다 큰 반도체 웨이퍼로의 입자침착)

  • Song, Gen-Soo;Yoo, Kyung-Hoon;Lee, Kun-Hyung
    • Particle and aerosol research
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    • v.5 no.1
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    • pp.17-27
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    • 2009
  • Particle deposition on a semiconductor wafer larger than 100 mm was studied experimentally and numerically. Particularly the electrostatic effect on particle deposition velocity was investigated. The experimental apparatus consisted of a particle generation system, a particle deposition chamber and a wafer surface scanner. Experimental data of particle deposition velocity were obtained for a semiconductor wafer of 200 mm diameter with the applied voltage of 5,000 V and PSL particles of the sizes between 83 and 495 nm. The experimental data of particle deposition velocity were compared with the present numerical results and the existing experimental data for a 100 mm wafer by Ye et al. (1991) and Opiolka et al. (1994). The present numerical method took into consideration the particle transport mechanisms of convection, Brownian diffusion, gravitational settling and electrostatic attraction in an Eulerian frame of reference. Based on the comparison of the present experimental and numerical results with the existing experimental results the present experimental method for a 200 mm semiconductor wafer was found to be able to present reasonable data.

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