• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2004.07b
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• pp.886-889
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• 2004

격자전극을 가진 질화탄소막을 이용하여 새로운 습도센서를 개발하였다. 결정성 질화탄소막의 감습 특성을 조사하고, 광범위한 상대습도($10%\sim90%$)에 대해 민감한 임피던스와 커패시턴스 의존도를 보였다. 특히 격자전극은 습기의 자유로운 흡 탈착을 용이 하게 하여 센서의 히스테리시스를 줄였다. 또한, 질화탄소막은 물리, 화학적으로 안정한 물질이므로 고온, 고습 및 화학적으로 열악한 환경 속에서도 뛰어난 특성 을 나타내었다.

• Proceedings of the Korean Society Of Semiconductor Equipment Technology
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• 2003.05a
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• pp.106-111
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• 2003

Tantalum nitride(TaN) films were deposited by atomic layer deposition(ALD) and plasma assisted atomic layer deposition(PAALD). The deposition of the TaN thin film has been performed using pentakis (ethylmethlyamino) tantalum (PEMAT) and ammonia($NH_3$) as precursors at temperature of $250^{\circ}C$, where the temperature was proven to be ALD window for TaN deposition from our previous experiments. The PAALD deposited TaN film shows better physical properties than thermal ALD deposited TaN film, due to its higher density$(~11.59 g/\textrm{cm}^3$) and lower carbon(~ 3 atomic %) and oxygen(~ 4 atomic %) concentration of impurities.

• Proceedings of the Korean Vacuum Society Conference
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• 2012.02a
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• pp.377-377
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• 2012

Microprocessor technology now relies on copper for most of its electrical interconnections. Because of the high diffusivity of copper, Atomic layer deposition (ALD) $TaN_x$ is used as a diffusion barrier to prevent copper diffusion into the Si or $SiO_2$. Another problem with copper is that it has weak adhesion to most materials. Strong adhesion to copper is an essential characteristic for the new barrier layer because copper films prepared by electroplating peel off easily in the damascene process. Thus adhesion-enhancing layer of cobalt is placed between the $TaN_x$ and the copper. Because, cobalt has strong adhesion to the copper layer and possible seedless electro-plating of copper. Until now, metal film has generally been deposited by physical vapor deposition. However, one draw-back of this method is poor step coverage in applications of ultralarge-scale integration metallization technology. Metal organic chemical vapor deposition (MOCVD) is a good approach to address this problem. In addition, the MOCVD method has several advantages, such as conformal coverage, uniform deposition over large substrate areas and less substrate damage. For this reasons, cobalt films have been studied using MOCVD and various metal-organic precursors. In this study, we used $C_{12}H_{10}O_6(Co)_2$ (dicobalt hexacarbonyl tert-butylacetylene, CCTBA) as a cobalt precursor because of its high vapor pressure and volatility, a liquid state and its excellent thermal stability under normal conditions. Furthermore, the cobalt film was also deposited at various $H_2/NH_3$ gas ratio(1, 1:1,2,6,8) producing pure cobalt thin films with excellent conformality. Compared to MOCVD cobalt using $H_2$ gas as a reactant, the cobalt thin film deposited by MOCVD using $H_2$ with $NH_3$ showed a low roughness, a low resistivity, and a low carbon impurity. It was found that Co/$TaN_x$ film can achieve a low resistivity of $90{\mu}{\Omega}-cm$, a low root-mean-square roughness of 0.97 nm at a growth temperature of $150^{\circ}C$ and a low carbon impurity of 4~6% carbon concentration.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.02a
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• pp.538-539
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• 2013

여러 장점으로 인해 OLED는 디스플레이 및 조명 등 적용분야가 넓어지고 있지만, 수분 및 산소에 취약하여 그 수명이 제한되는 단점이 있다. 이를 해결하고자 현재까지는 glass cap을 이용한 encapsulation 기술이 적용되고 있지만, flexible 기판에 적용하지 못하는 문제가 있다. 이러한 문제를 해결하고자 여러 가지 thin film encapsulation 기술이 적용되고 있으나 보다 신뢰성이 높은 기술의 개발이 절실한 때이다. Encapsulation 무기 박막 물질로서 $Si_3N_4$ 박막은 PE-CVD (Plasma Enhanced Chemical Vapor Deposition) 등의 박막 증착법을 사용한 많은 연구가 진행되어, 저온에서의 좋은 품질의 박막 증착이 가능하지만, 100도 이하의 thermal budget을 갖는 OLED Encapsulation에 사용하기에는 충분하지 않았다. CVD 박막의 특성을 더욱 개선하기 위해 최근 ALD (Atomic Layer Deposition) 방법을 통한 $Al_2O_3$ film 증착 방법이 연구되고 있지만, 낮은 증착 속도로 인해 양산에 걸림돌이 되고 있다. 본 연구에서는 또 다른 해결책으로서 Digital CVD 방법을 이용한 양질의 $Si_3N_4$ 박막의 증착을 연구하였다. 이것은 ALD 증착법과 유사하며, 1st step에서 PECVD 방법으로 4~5 ${\AA}$의 얇은 silicon 박막을 증착하고, 2nd step에서 nitrogen plasma를 이용하여 질화 반응을 진행하고, 이러한 cycle을 원하는 두께가 될 때까지 반복적으로 진행된다. 이 때 1 cycle 당 증착속도는 7 ${\AA}$/cycle 정도였다. 최적의 증착 방법과 조건으로 기존의 CVD $Si_3N_4$ 박막 대비 1/5 이하로 pinhole을 최소화 할 수는 있지만 완벽하게 제거하기는 힘든 문제가 있고, 이를 해결하기 위한 개선을 위한 접근 방법이 필요하다고 판단하였다. 본 연구에서는 무기물 박막인 carbon nitride를 이용한 SiN/C:N multilayer 증착 연구를 진행하였다. Fig. 1은 CVD 조건으로 증착된 두께 750 nm SiN film에서 여러 층의 C:N film layer를 삽입했을 때, 38 시간의 85%/$85^{\circ}C$ 가속실험에 따라 OLED의 발광 사진이다. 그림에서 볼 수 있듯이 C:N 층을 삽입하고 또한 그 박막의 수가 증가함에 따라서 OLED에 대한 encapsulation 특성이 크게 개선됨을 확인할 수 있다.

• Journal of the Korean Magnetics Society
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• v.16 no.1
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• pp.75-78
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• 2006

In case of contacts between semiconductor and metal in semiconductor circuits, they become unstable because of thermal budget. To prevent these problems, we use diffusion barrier that has a good thermal stability between metal and semiconductor. So we consider the diffusion barrier to prevent the increase of contact resistance between the interfaces of metals and semiconductors, and the increase of resistance and the reaction between the interfaces. In this paper we deposited tungsten boron carbon nitride (W-B-C-N) thin film on silicon substrate. The impurities of the $1000\;{\AA}-thick$ W-B-C-N thin films provide stuffing effect for preventing the inter-diffusion between metal thin films $(Cu-2000\;{\AA})$ and silicon during the high temperature $(700\~1000^{\circ}C)$ annealing process.

• Proceedings of the Korea Association of Crystal Growth Conference
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• 1996.06a
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• pp.75-87
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• 1996

This review is presented under the following headings: 1.Introduction 1.1 Brief review of the properties of AlN 1.2 Historical survey of work on ceramic and single crystal AlN 2.Thermochemical background 3.Crystal growth 4.Doping 5.Potential applications and future work The known properties of AlN which make it of interest for various are discussed briefly. The properties include chemical stability, crystal structure and lattice constants, refractive indices and other optical properties, dielectric constant, surface acoustic wave velocity and thermal conductivity. The history of work in single crystals, thin films and ceramics are outlined and the thermochemistry of AlN reviewed together with some of the relevant properties of aluminium and nitrogen; the problems encountered in growing crystals of AlN are shown to arise directly from these thermochemical relationships. Methods have been reported in the literature for growing AlN crystals from melts, solution and vapour and these methods are compared critically. It is proposed that the only practicable approach to the growth of AlN is by vapour phase methods. All vapour based procedures share the share the same problems: $.$the difficulty of preventing contamination by oxygen & carbon $.$the high bond energy of molecular nitrogen $.$the refractory nature of AlN (melting point~3073K at 100ats.) $.$the high reactivity of Al at high temperatures It is shown that the growth of epitactic layers and polycrystalline layers present additional problems: $.$chemical incompatibility of substrates $.$crystallographic mismatch of substrates $.$thermal mismatch of substrates The result of all these problems is that there is no good substrate material for the growth of AlN layers. Organometallic precursors which contain an Al-N bond have been used recently to deposit AlN layers but organometallic precursors gave the disadvantage of giving significant carbon contamination. Organometallic precursors which contain an Al-N bound have been used recently to deposit AlN layers but organometallic precursors have the disadvantage of giving significant carbon contamination. It is conclude that progress in the application of AlN to optical and electronic devices will be made only if considerable effort is devoted to the growth of larges, pure (and particularly, oxygen-free) crystals. Progress in applications of epi-layers and ceramic AlN would almost certainly be assisted also by the availability of more reliable data on the pure material. The essential features of any stategy for the growth of AlN from the vapour are outlined and discussed.

• Journal of the Korean Ceramic Society
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• v.53 no.4
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• pp.393-399
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• 2016

We have successfully fabricated 3D (3-dimensional) nanostructures of $TiO_2$ coated with a $g-C_3N_4$ layer via hydrothermal and sintering methods to enhance photoelectrochemical (PEC) performance. Due to the coupling of $TiO_2$ and $g-C_3N_4$, the nanostructures exhibited good performance as the higher conduction band of $g-C_3N_4$, which can be combined with $TiO_2$. To fabricate 3D nanostructures of $g-C_3N_4/TiO_2$, $TiO_2$ was first grown as a double layer structure on FTO (Fluorine-doped tin oxide) substrate at $150^{\circ}C$ for 3 h. After this, the $g-C_3N_4$ layer was coated on the $TiO_2$ film at $520^{\circ}C$ for 4 h. As-prepared samples were varied according to loading of melamine powder, with values of loading of 0.25 g, 0.5 g, 0.75 g, and 1 g. From SEM and TEM analysis, it was possible to clearly observe the 3D sample morphologies. From the PEC measurement, 0.5 g of $g-C_3N_4/TiO_2$ film was found to exhibit the highest current density of $0.12mA/cm^2$, along with a long-term stability of 5 h. Compared to the pristine $TiO_2$, and to the 0.25 g, 0.75 g, and 1 g $g-C_3N_4/TiO_2$ films, the 0.5 g of $g-C_3N_4/TiO_2$ sample was coated with a thin $g-C_3N_4$ layer that caused separation of the electrons and the holes; this led to a decreasing recombination. This unique structure can be used in photoelectrochemical applications.