• 제목/요약/키워드: $CH_4$/Ar

검색결과 167건 처리시간 0.023초

하이브리드 코팅 시스템으로 제조된 초고경도 Ti-Si-C-N 코팅막의 기계적 특성 평가 (Mechanical evaluation of superhard Ti-Si-C-N coatings prepared by a hybrid coating system)

  • 강신후;강명창;김광호
    • 한국소성가공학회:학술대회논문집
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    • 한국소성가공학회 2005년도 추계학술대회 논문집
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    • pp.178-181
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    • 2005
  • Quaternary Ti-Si-C-N coatings were deposited on WC-Co substrates by a hybrid coating system of arc ion plating (AIP) and sputtering techniques using Ti and Si targets, in an $Ar/N_2/CH_4$ gaseous mixture. The crystallinity, bending status, and microstructure of the Ti-Si-C-N coatings were measured by X-ray diffractometer (XRD) and X-ray photoelectron spectroscope (XPS), The micro-hardness of Ti(C,N) and Ti-Si-N coatings were about 30 and 40 GPa, respectively. As the Si was incorporated into Ti(C,N) coatings, the Ti-Si-C-N coatings having Si content of $8.9\;at.\%$ showed the maximum hardness value of about 55 GPa. In this work, the microstructure and mechanical properties of Ti-Si-C-N coatings were systematically investigated.

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CVD 다이아몬드 박막 기판의 방열 특성 (Heat Spreading Characteristics of CVD Diamond Film Substrate)

  • 임종환;강찬형
    • 한국표면공학회:학술대회논문집
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    • 한국표면공학회 2015년도 추계학술대회 논문집
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    • pp.305-305
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    • 2015
  • 알루미늄 방열판 위에 MPCVD(Microwave Plasma Enhanced Chemical Vapor Deposition) 장치를 이용하여 DC 바이어스 전압을 기판에 인가하면서 $Ar+CH_4$ 가스 분위기에서 증착한 나노결정질 다이아몬드(Nanocrystalline Diamond; NCD) 박막의 방열 특성을 평가하였다. XRD와 Raman spectroscopy를 이용하여 증착된 박막이 NCD인지를 확인하였으며 FE-SEM 및 FIB로 박막의 표면 및 단면의 형상을 관찰하였다. 다이아몬드가 증착된 방열판에 LED를 부착하여 발열시키고 열유동측정기의 하나인 T3-ster를 사용하여 방열 특성을 분석하였다. 기존 알루미늄(Al) 기판(5.55 K/W)보다 다이아몬드 증착(Dia-Al) 기판(3.88 K/W)의 열저항 값이 현저히 작았다, 또한 LED 접합온도는 Dia-Al 기판이 Al 기판보다 약 $3.5^{\circ}C$만큼 낮았다. 적외선 열화상 카메라로 발열 중인 시편의 전면과 후면을 촬영한 결과, LED가 부착된 전면부에서는 최고 발열 부위(hot spot)의 면적이 Al 기판의 경우가 Dia-Al 기판보다 높았고, 후면부에서는 그 반대의 경향을 보였다. 이들 데이터로부터 다이아몬드 증착 방열판이 기존의 방열판보다 방열특성이 우수한 것으로 해석할 수 있으며, 다이아몬드 박막을 방열판으로 사용하면 LED의 사용 수명과 효율이 높아질 것으로 기대된다.

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기판 종류에 따른 나노결정질 다이아몬드 박막의 성장 거동 비교 (Comparison of the Growth Behavior Nanocrystalline Diamond Film on Different Substrates)

  • 박동배;나봉권;명재우;강찬형
    • 한국표면공학회:학술대회논문집
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    • 한국표면공학회 2013년도 춘계학술대회 논문집
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    • pp.124-124
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    • 2013
  • 마이크로웨이브 플라즈마 화학기상증착(MPCVD) 시스템을 이용하여 서로 다른 기판(Si,SiC,W,Ti) 위에 나노결정질 다이몬드 박막을 증착하였다. 공정압력, 마이크로웨이브 전력, $Ar/CH_4$,기판온도를 일정하게 놓고, 증착시간을 0.5,1,2h으로 변화시켜 박막의 성장과정을 관찰하였다. 기판 종류에 따라 성장 초기에 형성되는 입자의 시간이 달랐으며, 2h 이후에는 입자들이 서로 붙어 완전한 박막을 형성함을 관찰하였다. 같은 증착시간에서 서로 다른 기판을 비교하였을 때, W > (Si, SiC) > Ti 기판의 순이었다.

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Application of Molecular Simulation Techniques to Estimation of Gas Permeability in Zeolite Membranes

  • Takaba, Hiromitsu;Yamamoto, Atsushi;Nakao, Shin-Ichi
    • 한국막학회:학술대회논문집
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    • 한국막학회 2004년도 Proceedings of the second conference of aseanian membrane society
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    • pp.33-38
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    • 2004
  • Molecular modeling of gas permeation through zeolite membranes with/without intercrystalline region was carried out. Molecular dynamics (MD) and Monte Carlo (MC) simulations were performed to estimate the diffusion coefficient and adsorption parameters respectively, and our proposed combined method of molecular simulation techniques with a permeation theory (CMP) was used to estimate gas permeability. The calculated permeability of gases (Ar, He, Ne, $N_2$, $0_2$, $CH_4$) at 301 K for the single crystal membrane model was about one order of magnitude larger than the experiential values, although the dependence on the molecular weight of the permeating species agreed with experiments. On the other hand, the estimated permeability using the diffusivity and adsorption parameters of the intercrystalline region model was in good agreement with the experiments. The consistency between experiments and the estimated values means the importance of considering the intercrystalline region and the validity of CMP method to predict the performance of zeolite membranes.

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n형 GaN의 doping 농도에 따르는 건식 식각 손상 (Doping-level dependent dry-etch damage of in n-type GaN)

  • 이지면
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2004년도 하계학술대회 논문집 Vol.5 No.1
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    • pp.417-420
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    • 2004
  • The electrical effects of dry-etch on n-type GaN by an inductively coupled $Cl_2/CH_4/H_2/Ar$ plasma were investigated as a function of ion energy, by means of ohmic and Schottky metallization method. The specific contact resistivity(${\rho}_c$) of ohmic contact was decreased, while the leakage current in Schottky diode was increased with increasing ion energy due to the preferential sputtering of nitrogen. At a higher rf power, an additional effect of damage was found on the etched sample, which was sensitive to the dopant concentration in terms of the ${\rho}_c$ of ohmic contact. This was attributed to the effects such as the formation of deep acceptor as well as the electron-enriched surface layer within the depletion layer. Furthermore, thermal annealing process enhanced the ohmic and Schottky property of heavily damaged surface.

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PECVD법에 의해 증착된 Ti-B-C코팅막 내의 보론함량과 증착온도에 따른 미세구조 및 기계적 물성의 변화 (The Effect of Boron Content and Deposition Temperature on the Microstructure and Mechanical Property of Ti-B-C Coating Prepared by Plasma-enhanced Chemical Vapor Deposition)

  • 옥정태;송풍근;김광호
    • 한국표면공학회지
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    • 제38권3호
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    • pp.106-111
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    • 2005
  • Ternary Ti-B-C coatings were synthesized on WC-Co and Si wafers substrates by a PECVD technique using a gaseous mixture of $TiCl_4,\;BCl_3,\;CH_4,\;Ar,\;and\; H_2$. The effects of deposition variables such as substrate temperature, gas ratio, $R_x=[BCl_3/(CH_4+BCl_3)]$ on the microstructure and mechanical properties of Ti-B-C coatings were investigated. From our instrumental analyses, the synthesized Ti-B-C coatings was confirmed to be composites consisting of nanocrystallites TiC, quasi-amorphous TiB2, and amorphous carbon at low boron content, on the contrary, nanocrystallites $TiB_2$, quasi-amorphous TiC, and amorphous carbon at relatively high boron content. The microhardness of the Ti-B-C coatings increased from $\~23 GPa$ of TiC to $\~38 GPa$ of $Ti_{0.33}B_{0.55}C_{0.11}$ coatings with increasing the boron content. The $Ti_{0.33}B_{0.55}C_{0.11}$ coatings showed lower average friction coefficient of 0.45, in addition, it showed relatively better wear behavior compared to other binary coatings of $TiB_2$ and TiC. The microstruture and microhardness value of Ti-B-C coatings were largely depend on the deposition temperature.

메탄의 산화성 짝지음 반응에 관한 연구 (Oxidative Coupling Reaction of Methane)

  • 김상범;함현식
    • 한국응용과학기술학회지
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    • 제13권1호
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    • pp.67-74
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    • 1996
  • This study was conducted to find a catalyst system which has high conversion and selectivity for the oxidative coupling of methane to produce ethane and ethylene. Various catalysts were tested in a fixed bed reactor ar $750^{\circ}C$, 1 atm, and the feed ratio($CH_4/O_2$) of 2/1. Under the reaction condition, 10wt%$PbSO_4/MgO$ catalyst showed the highest catalytic activity : methane conversion, $C_2$ selectivity and yield were 50, 40 and 20%, respectively. Catalysts containing sulfate compounds, 10wt%$PbSO_4/MgO$, 10wt%$MgSO_4/MgO$ and $Na_2SO_4/MgO$ revealed a moderate methane conversions such as 38, 50 and 50%, respectively and low $C_2$ selectivities such as 18, 5 and 9%, respectively. Catalysts containing carbonate compounds, 10wt%$PbCO_3/MgO$, 10wt%$Li_2CO_3/MgO$ and $NaCO_3/MgO$, also showed a moderate methane conversions such as 64, 44 and 51%, respectively and low $C_2$ selectivities such as 5, 6 and 2%, respectively. With the existence of chlorine and mercury, $C_2$ selectivity was decreased.

Synthesis of Graphene on Hexagonal Boron Nitride by Low Pressure Chemical Vapor

  • Han, Jae-Hyun;Yeo, Jong-Souk
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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    • pp.391-392
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    • 2012
  • Graphene is a perfectly two-dimensional (2D) atomic crystal which consists of sp2 bonded carbon atoms like a honeycomb lattice. With its unique structure, graphene provides outstanding electrical, mechanical, and optical properties, thus enabling wide variety of applications including a strong potential to extend the technology beyond the conventional Si based electronic materials. Currently, the widespread application for electrostatically switchable devices is limited by its characteristic of zero-energy gap and complex process in its synthesis. Several groups have investigated nanoribbon, strained, or nanomeshed graphenes to induce a band gap. Among various techniques to synthesize graphene, chemical vapor deposition (CVD) is suited to make relatively large scale growth of graphene layers. Direct growth of graphene on hexagonal boron nitride (h-BN) using CVD has gained much attention as the atomically smooth surface, relatively small lattice mismatch (~1.7%) of h-BN provides good quality graphene with high mobility. In addition, induced band gap of graphene on h-BN has been demonstrated to a meaningful value about ~0.5 eV.[1] In this paper, we report the synthesis of grpahene / h-BN bilayer in a chemical vapor deposition (CVD) process by controlling the gas flux ratio and deposition rate with temperature. The h-BN (99.99%) substrate, pure Ar as carrier gas, and $CH_4$ are used to grow graphene. The number of graphene layer grown on the h-BN tends to be proportional to growth time and $CH_4$ gas flow rate. Epitaxially grown graphene on h-BN are characterized by scanning electron microscopy, atomic force microscopy, and Raman spectroscopy.

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Synthesis of High-quality Graphene by Inductively-coupled Plasma-enhanced Chemical Vapor Deposition

  • Lam, Van Nang;Kumar, Challa Kiran;Park, Nam-Kyu;Arepalli, Vinaya Kumar;Kim, Eui-Tae
    • 한국재료학회:학술대회논문집
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    • 한국재료학회 2011년도 추계학술발표대회
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    • pp.16.2-16.2
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    • 2011
  • Graphene has attracted significant attention due to its unique characteristics and promising nanoelectronic device applications. For practical device applications, it is essential to synthesize high-quality and large-area graphene films. Graphene has been synthesized by eloborated mechanical exfoliation of highly oriented pyrolytic graphite, chemical reduction of exfoliated grahene oxide, thermal decomposition of silicon carbide, and chemical vapor deposition (CVD) on metal substrates such as Ni, Cu, Ru etc. The CVD has advantages over some of other methods in terms of mass production on large-areas substrates and it can be easily separated from the metal substrate and transferred to other desired substrates. Especially, plasma-enhanced CVD (PECVD) can be very efficient to synthesize high-quality graphene. Little information is available on the synthesis of graphene by PECVD even though PECVD has been demonstrated to be successful in synthesizing various carbon nanostructures such as carbon nanotubes and nanosheets. In this study, we synthesized graphene on $Ni/SiO_2/Si$ and Cu plate substrates with CH4 diluted in $Ar/H_2$ (10%) by using an inductively-coupled PECVD (ICPCVD). High-quality graphene was synthesized at as low as $700^{\circ}C$ with 600 W of plasma power while graphene layer was not formed without plasma. The growth rate of graphene was so fast that graphene films fully covered on substrate surface just for few seconds $CH_4$ gas supply. The transferred graphene films on glass substrates has a transmittance at 550 nm is higher 94%, indicating 1~3 monolayers of graphene were formed. FETs based on the grapheme films transferred to $Si/SiO_2$ substrates revealed a p-type. We will further discuss the synthesis of graphene and doped graphene by ICPVCD and their characteristics.

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DC Bias가 다결정 실리콘 기판 위 나노결정 다이아몬드 박막의 성장에 미치는 영향 (Effect of DC Bias on the Growth of Nanocrystalline Diamond Film over Poly-Silicon Substrate)

  • 김선태;강찬형
    • 한국표면공학회:학술대회논문집
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    • 한국표면공학회 2016년도 추계학술대회 논문집
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    • pp.180-180
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    • 2016
  • 보론이 도핑된 $3{\times}3cm$ 크기의 p 형 다결정 실리콘 기판의 표면을 경면연마한 후, 다이아몬드 입자의 seeding을 위해 슬러리 중 다이아몬드 분말의 입도를 5 nm로 고정하고 초음파 전처리 공정을 진행한 후, 다이아몬드 박막을 증착하였다. 다이아몬드 증착은 Microwave Plasma Chemical Vapor Deposition 장비를 이용하였으며, 공정 조건은 초기 진공 $10{\times}10^{-3}Torr$, 공정 가스 비율 $Ar:CH_4=200:2$, 가스 유량 202 sccm, 공정압력 90 Torr, 마이크로웨이브 파워 600 W, 기판 온도 $600^{\circ}C$이었다. 기판에 DC bias 전압을 인가하는 것을 공정 변수로 하여 0, -50, -100, -150, -200 V로 변화시켜가며, 0.5, 1, 2, 4 h 동안 증착을 진행하였다. 주사전자현미경과 XRD, AFM, 접촉각 측정 장비를 이용하여 증착된 다이아몬드 입자와 막의 특성을 분석하였다. 각 bias 조건에서 초기에는 다이아몬드 입자가 형성되어 성장되었다가 시간이 증가될수록 연속적인 다이아몬드 막이 형성되었다. Table 1은 각 bias 조건에서 증착 시간을 4 h까지 변화시키면서 얻은 다이아몬드 입자 또는 박막의 높이(두께)를 나타낸 것이다. 2 h까지의 공정 초기에는 bias 조건의 영향을 파악하기 어려운데, 이는 bias에 의한 과도한 이온포격으로 입자가 박막으로의 성장에 저해를 받는 것으로 사료된다. 증착시간이 4 h가 경과하면서 -150 V 조건에서 가장 두꺼운 막이 성장되었다. 이는 기판 표면을 덮은 다이아몬드 박막 위에서 이차 핵생성이 bias에 의해 촉진되기 때문으로 해석된다. -200 V의 조건에서는 오히려 막의 성장이 더 느렸는데, 이는 Fig. 1에 보이듯이 과도한 이온포격으로 Si/diamond 계면에서 기공이 형성된 것과 연관이 있는 것으로 보인다.

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