• Title/Summary/Keyword: LCVD

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The Study on Thin Film Fabrication using UHV-LCVD System (I) (UHV-LCVD 장치를 이용한 박막제작에 관한 연구 (I) - 장치 제작을 중심으로 -)

  • Choi, Won-Kook;Yun, Dug-Ju;Gong, Byung-In;Kim, Chang-Hyun;Whang, Chung-Nam;Jeong, Kwang-Ho
    • Journal of the Korean Vacuum Society
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    • v.2 no.2
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    • pp.255-260
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    • 1993
  • UHV-LCVD system was constructed for high quality silicon nitride thin film fabrication. This system consisted of a reaction chamber, an introduction chamber with sample load lock entry, a carbinet for gas manipulation controlling gas flow, a $CO_2$ laser and a Fourier transform mass spectrometer. Although the UHV-LCVD system construction was more sophisticated than low pressure CVD, highly pure thin films were fabricated by controlling gas mixing ratio and flow rate in ultra high vacuum surroundings.

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Electrical Properties of Laser CVD Silicon Nitride Film (Laser CVD SiN막의 전기적 특성)

  • Kim, Yong-Woo;Kim, Sang-Wook;Park, Jong-Wook;Kim, Chun-Sub;Sung, Yung-Kwon
    • Proceedings of the KIEE Conference
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    • 1990.11a
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    • pp.85-87
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    • 1990
  • Silicon nitride film was deposited on a silicon wafer using a laser CVD(LCVD) technique, which is based on direct photolysis of $SiH_4/NH_3$ gas mixture by ArF laser beam(${\lambda}=193\;nm$). The refractive index of deposited SiN film is 1.9 at the temperature of $300^{\circ}C$, pressure of 5 torr. The breakdown field strength of LCVD SiN film was 10MV/cm. In IR spectrum, the absorption peak of Si-H, N-H, and Si-N is detected and it is shown that hydrogen is included in SiN film. From analysis of absorption band. it is calculated that density of Si-H, N-H bond is higher than $5{\times}10^{22}cm^{-3}$. LCVD MIS capacitor and PECVD MIS capacitor have injection-type hysteresis but it is known that hysteresis loss of LCVD MIS capacitor is smaller than that of PECVD MIS capacitor. It means that Interface state density of LCVD capacitor is smaller than that of PECVD capacitor. In addition, the flatband voltage($V_{FB}$) of LCVD is smaller than that of PECVD capacitor. And it means that fixed charged density($Q_{FIX}$) of LCVD capacitor is smaller than that of PECVD MIS capacitor.

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A Study on the Fabrication of LCVD System and Characteristics of Silicon Nitride Thin Film Deposited by the System (LCVD법을 이용한 박막성장장치의 제작 및 그 장치를 이용하여 제작한 Silicon Nitride 박막의 특성 연구)

  • 유동선;김일곤;이호섭;정광호
    • Journal of the Korean Vacuum Society
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    • v.2 no.3
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    • pp.368-373
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    • 1993
  • LCVD법에 의한 박막성장장치를 제작하였다. 제작한 CO2 레이저는 CO2 : N2 : He이 1 : 1 : 8로 혼합된 가스를 사용하였으며 최대 출력은 60W였고 혼합가스의 유량이 20l/min, 방전전류 40mAdlfEo 50W의 비교적 안정된 출력을 얻을 수 있었다. 반응실의 기초 진공은 1$\times$10-6torr였으며 레이저를 기판에 수직 혹은 수평으로 조사할 수 있도록 설계하였다. 제작된 장치로 SiH4 및 NH3를 재료로 하여 실리콘 및 quartz 기판위에 silicon nitride 박막을 증착하였다. 박막 생장시 가스를 흘리는 방식보다 가스를 채워놓고 하는 방식이 낮은 레이저 출력하에서 균일한 박막을 얻는데 효율적이라는 것을 발견하였다. 출력 55W의 레이저를 실리콘 기판에 5분간 조사하였을 때 최대 두께1.5$mu extrm{m}$의 박막을 얻었으며 quartz 기판위에는 출력 4W, 조사시간 6분에서 두께가 약 1$\mu\textrm{m}$인 비교적 균질의 박막을 얻을 수 있었다. FT-IR 및 XPS 분석 결과 SiH4와 NH3의 혼합비가 1 : 12일 때 비교적 nitride화가 잘 된 박막이 얻어졌음을 알았다.

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Wear out in electrically stressed LCVD silicon nitride films (Laser CVD silicon nitride막의 wear out)

  • Kim, Chun-Sub;Kwon, Bong-Jae;Kim, Yong-Woo;Kim, Seong-Jeen;Sung, Yung-Kwon
    • Proceedings of the KIEE Conference
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    • 1990.11a
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    • pp.115-118
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    • 1990
  • Recently, it has been reported that the Insulating films deposited by PECVD show some degradation under somewhat high electric field. In this paper, we Introduce silicon nitride films deposited by LCVD, and evaluate the breakdown and wear-out of these films by TDDB test. Further, failure times against electric field are examined and acceleration factors $\gamma$ are obtained for each case. As a result, it is shown that the breakdown and wear-out limitation for these films is improved.

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Experimental Study of the Growth of the SiC Rod using LCVD (LCVD를 이용한 SiC 로드 성장에 관한 실험적 연구)

  • Ryu, Jae-Eun;Lee, Byeong-Ro;Lee, Young-Lim
    • Proceedings of the KSME Conference
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    • 2003.04a
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    • pp.1615-1620
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    • 2003
  • The purpose of the study is not only to establish experimental system for laser chemical vapor deposition but also to find the characteristics of SiC rod growth that is the beginning step in developing technology of 3 dimensional prototyping with laser chemical vapor deposition. In this study, SiC rod was generated with varying TMS pressure for 5 minutes. Deposition rates with varying TMS pressure, shapes of rods, surface roughness and component organization were investigated, in particular.

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Fabrication of micro carbon structures using laser-induced chemical vapor deposition and Raman spectroscopic analysis (레이저 국소증착에 의한 탄소 미세 구조물 제조 및 분광분석)

  • ;;J. Senthil Selvan
    • Laser Solutions
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    • v.5 no.2
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    • pp.17-22
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    • 2002
  • Characteristics of micro carbon structures fabricated with laser-induced chemical vapor deposition (LCVD) are investigated. An argon ion laser (λ=514.5nm) and ethylene gas were utilized as the energy source and precursor, respectively. The laser beam was focused onto a graphite substrate to produce carbon deposit through thermal decomposition of the precursor. Average growth rate of a carbon rod increased for increasing laser power and pressure. Micro carbon rods with good surface quality were obtained at near the threshold condition. Micro carbon rods with aspect ratio of about 100 and micro tubular structures were fabricated to demonstrate the possible application of this method to the fabrication of three-dimensional microstructures. Laser Raman spectroscopic analysis of the micro carbon structures revealed that the carbon rods are consisting of amorphous carbon.

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Fabrication of Micro Carbon Structures and Patterns with Laser-assisted Chemical Vapor Deposition (레이저 국소증착을 통한 미세 탄소구조물 및 패턴 제조)

  • 정성호;김진범;이선규;이종현
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 2002.05a
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    • pp.914-917
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    • 2002
  • Fabrication of micro carbon structures and patterns using laser-assisted chemical vapor deposition is studied. Argon ion laser and ethylene were used to grow micro carbon rod through pyrolytic decomposition of the reaction gas. The influence of reaction gas pressure and incident laser power on the diameter and growth rate of the micro carbon rod was experimentally investigated. The diameter of micro carbon rods increases linearly with respect to the laser power but is almost independent of the reaction gas pressure. Growth rate of the rod changes little with gas pressure when the laser power remains below 1W. When the carbon rod was grown at near threshold laser power, a very smooth surface is obtained on the rod. By continuously moving the focusing lens in the direction of growth, a micro carbon rod with a diameter of 28 ${\mu}{\textrm}{m}$ and aspect ratio of 100 was fabricated.

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Epitaxial Growth of GaAs/GaAs and GaAs/Si by LCVD (레이저 CVD를 이용한 GaAs/GaAs 및 GaAs/Si 결정성장연구)

  • Choi, W.L.;Ku, J.K.;Chung, J.W.;Kwon, O.
    • Proceedings of the KIEE Conference
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    • 1989.11a
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    • pp.79-82
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    • 1989
  • We studied the epitaxial growth of GaAs/GaAs and GaAs/Si by Laser CVD with 193nm ArF pulsed excimer laser. The source gases of TMGa and AsC13 or TMGa-TMAs adducts are mixed with H2, and photolyzed above the substrate which is heated up to around 300$^{\circ}C$. Then the photolyzed atoms are deposited on the silicon or GaAs substrate. The deposited films are analyzed with ESKA depth profiling and X-ray differaction method, which shows that the films on Si and GaAs are stoichiometric and crystalized at such a low temperature. We show a clear evidence for the epitaxial growth of GaAs on Si or GaAs on GaAs at low temperature by excimer laser CVD.

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Single-phase Gallium Nitride on Sapphire with buffering AlN layer by Laser-induced CVD

  • Hwang Jin-Soo;Lee Sun-Sook;Chong Paul-Joe
    • Bulletin of the Korean Chemical Society
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    • v.15 no.1
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    • pp.28-33
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    • 1994
  • The laser-assisted chemical vapor deposition (LCVD) is described, by which the growth of single-phase GaN epitaxy is achieved at lower temperatures. Trimethylgallium (TMG) and ammonia are used as source gases to deposit the epitaxial films of GaN under the irradiation of ArF excimer laser (193 nm). The as-grown deposits are obtained on c-face sapphire surface near 700$^{\circ}$C, which is substantially reduced, relative to the temperatures in conventional thermolytic processes. To overcome the lattice mismatch between c-face sapphire and GaN ad-layer, aluminum nitride(AlN) is predeposited as buffer layer prior to the deposition of GaN. The gas phase interaction is monitored by means of quadrupole mass analyzer (QMA). The stoichiometric deposition is ascertained by X-ray photoelectron spectroscopy (XPS). The GaN deposits thus obtained are characterized by X-ray diffractometer (XRD), scanning electron microscopy (SEM) and van der Pauw method.