• Title/Summary/Keyword: Vapor Deposition Process

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Growth of Amorphous SiOx Nanowires by Thermal Chemical Vapor Deposition Method (열화학 기상 증착법에 의한 비정질 SiOx 나노와이어의 성장)

  • Kim, Ki-Chul
    • Journal of Convergence for Information Technology
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    • v.7 no.5
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    • pp.123-128
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    • 2017
  • Nanostructured materials have received attention due to their unique electronic, optical, optoelectrical, and magnetic properties as a results of their large surface-to-volume ratio and quantum confinement effects. Thermal chemical vapor deposition process has attracted much attention due to the synthesis capability of various structured nanomaterials during the growth of nanostructures. In this study, silicon oxide nanowires were grown on Si\$SiO_2$(300 nm)\Pt(5~40 nm) substrates by two-zone thermal chemical vapor deposition with the source material $TiO_2$ powder via vapor-liquid-solid process. The morphology and crystallographic properties of the grown silicon oxide nanowires were characterized by field-emission scanning electron microscope and transmission electron microscope. As results of analysis, the morphology, diameter and length, of the grown silicon oxide nanowires are depend on the thickness of the catalyst films. The grown silicon oxide nanowires exhibit amorphous phase.

The transparent and conducting tin oxide thin films by the remote plasma chemical vapor deposition (원격플라즈마화학증착에 의한 투명전도성 산화주석 박막)

  • 이흥수;윤천호;박정일;박광자
    • Journal of the Korean Vacuum Society
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    • v.7 no.1
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    • pp.43-50
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    • 1998
  • Transparent and conducting tin oxide films were prepared on Pyrex glass substrates by the remote plasma chemical vapor deposition (RPCVD). The main control variables of the RPCVD process included the deposition time, the flow rates of tetramethyltin, oxygen and argon, the radio-frequency power, and the substrate temperature. Dependence of the deposition rate, electric resistivity, optical transmittance and crystal structure on these parameters was systematically examined to prepare high qualities of tin oxide films and to better understand RPCVD process. The effect of those parameters on the properties of tin oxide films in complicatedly related on another. A tin oxide film parameters on the protimized deposition conditions exhibited deposition rate of 102 $\AA$/min, electric resistivity of $9.7\times 10^{-3}\Omega$cm and visible transmittance of ~80%.

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Large Area Bernal Stacked Bilayer Graphene Grown by Multi Heating Zone Low Pressure Chemical Vapor Deposition

  • Han, Jaehyun;Yeo, Jong-Souk
    • Proceedings of the Korean Vacuum Society Conference
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    • 2015.08a
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    • pp.239.2-239.2
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    • 2015
  • Graphene is a most interesting material due to its unique and outstanding properties. However, semi-metallic properties of graphene along with zero bandgap energy structure limit further application to optoelectronic devices. Recently, many researchers have shown that band gap can be induced in the Bernal stacked bilayer graphene. Several methods have been used for the controlled growth of the Bernal staked bilayer graphene, but it is still challenging to control the growth process. In this paper, we synthesize the large area Bernal stacked bilayer graphene using multi heating zone low pressure chemical vapor deposition (LPCVD). The synthesized bilayer graphenes are characterized by Raman spectroscopy, optical microscope (OM), scanning electron microscopy (SEM). High resolution transmission electron microscopy (HRTEM) is used for the observation of atomic resolution image of the graphene layers.

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The geometry change of carbon nanofilaments by SF6 incorporation in a thermal chemical vapor deposition system

  • Kim, Sung-Hoon
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.21 no.3
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    • pp.119-123
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    • 2011
  • Carbon nanotilaments (CNFs) could be synthesized on nickel catalyst layer-deposited silicon oxide substrate using $C_2H_2$ and$H_2$ as source gases under thermal chemical vapor deposition system. By the incorporation of $SF_6$ as a cyclic modulation manner, the geometries of carbon coils-related materials, such as nano-sized coil and wave-like nano-sized coil could be observed on the substrate. The characteristics (formation density and morphology) of as-grown CNFs with or without $SF_6$ incorporation were investigated. Diameter size reduction for the individual CNFs-related shape and the enhancement of the formation density of CNFs-related material could be achieved by the incorporation of $SF_6$ as a cyclic modulation manner. The cause for these results was discussed in association with the slightly increased etching ability by $SF_6$ addition and the sulfur role in SF 6 for the geometry change.

Fabrication of High Tc Superconducting Films by CVD Process

  • Lee, Sang-Heon
    • Transactions on Electrical and Electronic Materials
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    • v.5 no.3
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    • pp.120-121
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    • 2004
  • YBaCuO thick films were fabricated by plasma enhanced chemical vapor deposition, and the crystallinity and the superconducting properties were investigated. The growth temperature to obtain the thick films was decreased by around 150$^{\circ}C$ due to plasma enhancement. The zero resistivity temperatures for films grown at 590$^{\circ}C$ and 620$^{\circ}C$ were 55 and 80 K, respectively.

Fabrication of BSCCO Films using CVD Process

  • Lee, Sang-Heon
    • Transactions on Electrical and Electronic Materials
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    • v.5 no.4
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    • pp.158-160
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    • 2004
  • BiSrCaCuO thick films were fabricated by plasma enhanced chemical vapor deposition, and the crystallinity and the superconducting properties were investigated. The superconductivity was achieved at 20 K with an onset temperature of around 90 K in the film prepared at 72$0^{\circ}C$. From X ray diffraction analysis, the main superconducting phase in the films was the low Tc phase at 700∼75$0^{\circ}C$ and the high Tc phase at 750 ∼ 80$0^{\circ}C$.

Process Controllability and Stability in Organic Vapor Phase Deposition

  • Schwambera, M.;Gersdorff, M.;Reinhold, M.;Meyer, N.;Strauch, G.;Marheineke, B.;Heuken, M.;Zhou, T.X.;Ngo, T.;Brown, J.J.;Shtein, M.;Forrest, S.R.
    • 한국정보디스플레이학회:학술대회논문집
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    • 2004.08a
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    • pp.824-827
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    • 2004
  • High performance green $Ir(ppy)_3$-based phosphorescent OLEDs (PHOLEDs) have been fabricated by organic vapor phase deposition ($OVPD^{TM}$). In addition to demonstrating both efficiency and operational device lifetime comparable to devices built by vacuum thermal evaporation, we report on the controllability and stability of the $OVPD^{TM}$ process. Specifically, run-to-run and day-to-day deposition rate reproducibility of better than 2 % for three consecutive days is demonstrated.

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Neutral Beam assisted Chemical Vapor Deposition at Low Temperature for n-type Doped nano-crystalline silicon Thin Film

  • Jang, Jin-Nyeong;Lee, Dong-Hyeok;So, Hyeon-Uk;Yu, Seok-Jae;Lee, Bong-Ju;Hong, Mun-Pyo
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.52-52
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    • 2011
  • A novel deposition process for n-type nanocrystalline silicon (n-type nc-Si) thin films at room temperature has been developed by adopting the neutral beam assisted chemical vapor deposition (NBa-CVD). During formation of n-type nc-Si thin film by the NBa-CVD process with silicon reflector electrode at room temperature, the energetic particles could induce enhance doping efficiency and crystalline phase in polymorphous-Si thin films without additional heating on substrate; The dark conductivity and substrate temperature of P-doped polymorphous~nano crystalline silicon thin films increased with increasing the reflector bias. The NB energy heating substrate(but lower than $80^{\circ}C$ and increase doping efficiency. This low temperature processed doped nano-crystalline can address key problem in applications from flexible display backplane thin film transistor to flexible solar cell.

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Low Pressure Chemical Vapor Deposition of Silicon Carbide (탄화규소의 저압 화학증착)

  • 송진수;김영욱;김동주;최두진;이준근
    • Journal of the Korean Ceramic Society
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    • v.31 no.3
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    • pp.257-264
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    • 1994
  • The objectives of this study were to develop the low pressure chemical vapor deposition(LPCVD) process of SiC and to fabricate pure and dense SiC layer onto graphite substrate at low temperature. The deposition experiments were performed using the MTS-H2 system (30 torr) in the deposition temperature ranging from 100$0^{\circ}C$ to 120$0^{\circ}C$. The deposition rate of SiC was increased with the temperature. The rate controlling step can be classified from calculated results of the apparent thermal activation energy as follows; surface reaction below 110$0^{\circ}C$ and gas phase diffusion through a stagnant layer over 110$0^{\circ}C$. The deposited layer was $\beta$-SiC with a preferred orientation of (111) and the strongly faceted SiC deposits were observed over 115$0^{\circ}C$.

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In-situ magnetization measurements and ex-situ morphological analysis of electrodeposited cobalt onto chemical vapor deposition graphene/SiO2/Si

  • Franco, Vinicius C. De;Castro, Gustavo M.B.;Corredor, Jeaneth;Mendes, Daniel;Schmidt, Joao E.
    • Carbon letters
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    • v.21
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    • pp.16-22
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    • 2017
  • Cobalt was electrodeposited onto chemical vapor deposition (CVD) graphene/Si/$SiO_2$ substrates, during different time intervals, using an electrolyte solution containing a low concentration of cobalt sulfate. The intention was to investigate the details of the deposition process (and the dissolution process) and the resulting magnetic properties of the Co deposits on graphene. During and after electrodeposition, in-situ magnetic measurements were performed using an (AGFM). These were followed by ex situ morphological analysis of the samples with ${\Delta}t_{DEP}$ 30 and 100 s by atomic force microscopy in the non-contact mode on pristine CVD graphene/$SiO_2$/Si. We demonstrate that it is possible to electrodeposit Co onto graphene, and that in-situ magnetic measurements can also help in understanding details of the deposition process itself. The results show that the Co deposits are ferromagnetic with decreasing coercivity ($H_C$) and demonstrate increasing magnetization on saturation ($M_{SAT}$) and electric signal proportional to remanence ($M_r$), as a function of the amount of the electrodeposited Co. It was also found that, after the end of the dissolution process, a certain amount of cobalt remains on the graphene in oxide form (this was confirmed by X-ray photoelectron spectroscopy), as suggested by the magnetic measurements. This oxide tends to exhibit a limited asymptotic amount when cycling through the deposition/dissolution process for increasing deposition times, possibly indicating that the oxidation process is similar to the graphene surface chemistry.