• Journal of the Korean Institute of Telematics and Electronics D
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• v.36D no.7
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• pp.17-25
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• 1999

Tungsten nitride($WN_x$) films were deposited by PECVD method on silicon nitride($WSi_3N_4$) substrate. The characteristics of $WN_x$ film were investigated with changing various processing parameters ; substrate temperature, gas flow rate, rf power, and different nitrogen sources. The nitrogen composition in $WN_x$ film varied from 0 to 45% according to the $NH_3$ and $N_2$ flow rate. The highest deposition rate of 160 nm/min was obtained for the $NH_3$ gas and relatively low deposition rate of $WN_x$ films were formed by $N_2$ gas. $WN_x$ films deposited on $WSi_3N_4$ substrate had higher deposition rate than that of TiN and Si substrates. The purity of $WN_x$ film were analyzed by AES and higher purity $WN_x$ films were deposited using $NH_3$ gas. The XRD analysis indicates a phase transition from polycrystalline tungsten(W) to amorphous tungsten nitride($WN_x$), showing improved etching profile of $WN_x$ films Thick $WN_x$ films were deposited on various substrates such as Tin, NiCr and Al and maximum thickness of $1.6 {\mu}m$ was obtained on the Al adhesion layer.

• Journal of the Korean Ceramic Society
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• v.38 no.12
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• pp.1180-1186
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• 2001

W $O_3$-Sn $O_2$thin film sensors with approximately 1${\mu}{\textrm}{m}$ in thickness were fabricated by using a high-vacuum resistance-heating evaporator, were annealed at 50$0^{\circ}C$ for 4 hours in air, and then their crystallinities and surface microstructures were analyzed. As results of gas-sensing characteristics to oxidizing gas, N $O_2$, and reducing gas, CO, of 100 ppm, the highest gas sensitivities (S= $R_{gas}$/ $R_{air}$) were the W $O_3$thin-film sensor measured at 25$0^{\circ}C$ for N $O_2$(S≒1000) and the Sn $O_2$thin-film sensor measured at 15$0^{\circ}C$ to 25$0^{\circ}C$ range for CO (S≒0.25), respectively.ely.

• Journal of Sensor Science and Technology
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• v.8 no.3
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• pp.291-297
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• 1999

The plasma etching of tungsten thin films has been studied with $SF_6$ gas in RIE system. The etch rate of ${\alpha}$-phase W film with $SF_6$ gas plasma has been showed to depend strongly on process parameters ($SF_6$, $SF_6-N_2$ gas). Effect of $N_2$ addition and etching selectivity between W film and photoresist have also been studied in detail. Etching profiles between W film and photoresist were investigated by SEM. The compounds on W surface after $SF_6-N_2$ gas plasma treatment were examined by XPS and the concentration of F ions was detected by OES during plasma on.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2005.11a
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• pp.109-110
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• 2005

We have suggested sputtered W-C-N thin film for preventing thermal budget between semiconductor and metal. These results show that the W-C-N thin film has good thermal stability and low resistivity. In this study we newly suggested sputtered W-B-C-N thin diffusion barrier. In order to improve the characteristics, we examined the impurity behaviors as a function of nitrogen gas flow ratio. This thin film is able to prevent the interdiffusion during high temperature (700 to $1000^{\circ}C$) annealing process and has low resistivity ($\sim$200$\mu{\Omega}-cm$). Through the analysis of X-Ray diffraction, resistivity and XPS, we studied structure behavior of W-B-C-N diffusion barrier.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2006.06a
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• pp.114-115
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• 2006

반도체 기술이 초고집적화 되어감에 따라 공정에서 선폭이 줄어들고, 박막을 다층으로 제조하는 것이 중요하게 되었다. 이와 같은 제조 공정 하에서는 Si 기판과 금속 박막간의 확산이 커다란 문제로 부각되어 왔다. 특히 Cu는 높은 확산성에 의하여 Si 기판과 접합에서 많은 확산에 의한 문제가 발생하게 되며. 또한 선폭이 줄어듦에 따라 고열이 발생하여 실리콘으로 spiking이 발생하게 된다. 이를 방지하기 위하여 우리는 3개의 화합물로 구성된 Tungsten-Carbon-Nitrogen (W-C-N) 확산방지막을 사용하였다. 실험은 물리적 기상 증착법 (PVD)으로 질소비율을 변화하며 확산방지막을 증착하였고, 이를 여러 온도에서 열처리하여 X-ray Diffraction 분석을 하였다.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.6 no.3
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• pp.318-326
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• 1996

This study is to investigate a chemical vapor deposition technique of copper film which is expected to be more useful as metallizations of microcircuit fabrication. An experimental equipment was designed and set-up for this study, and a Cu-precursor used that is a metal-organic compound, named (hfac)Cu(I)VTMS ; (hevaflouoroacetylacetonate trimethyvinylsilane copper). Base pressure of the experimental system is in $10^{-6}$ Torr, and the chamber pressure and the substrate temperature can be controlled in the system. Before the deposition of copper thin film, tungsten or titanium nitride film was deposited onto the silicon wafer. Helium has been used as carrier gas to control the deposition rate. As a result, deposition rate was measured as $1,800\;{\AA}/min$ at $220^{\circ}C$ which is higher than the results of previous studies, and the average surface roughness was measured as about $200\;{\AA}$. A deposition selectivity was observed between W or TiN and $SiO_{2}$ substrates below $250^{\circ}C$, and optimum results are observed at $180^{\circ}C$ of substrate temperature and 0.8 Torr of chamber pressure.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.9 no.3
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• pp.273-279
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• 1999

The home-made hot wall epitaxy (HWE) system was utilized for GaN epitaxial layer growth on the Si(001) substrate. It was appeared that GaN epilayer grow with mixed phase of Zinc blende and Wurtzite structure from photoluminescence (PL) and x-ray diffraction (XRD) analysis at the room temperature. We found that intial growth layer has Wurtzite structure from photoluminescence (PL) and x-ray diffractio (XRD) analyses at the room temperature. Wefound that initial growth layer has Wurtzite structure when initial deposition time, the temperature of substrate and source are 4 min, $720^{\circ}C$ and $860^{\circ}C$ respectively, and at the epi growth process GaN, epilayer was grown with relatively stable Wurtzite structure when the temperature of substrate and source are $1020^{\circ}C$ and $910^{\circ}C$ respectively.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2008.06a
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• pp.155-155
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• 2008

계속되는 반도체 산업의 발달로 반도체 배선 공정에서는 Al을 대체할 배선 금속으로 Cu에 대한 관심이 집중되고, 일부 공정에서는 Al을 대신하여 사용하고 있다. 이러한 Cu는 Al에 비교하여 많은 장점을 가지고 있지만 Si 기판과 저온에서 쉽게 확산되는 큰 문제점을 가지고 있다. 따라서 이러한 문제를 해결하기 위한 방법으로 현재까지 연구된 대안으로는 Cu와 Si기판 사이에 확산방지막을 삽입하는 것이 대안으로 알려져 있다. 본 연구는 Cu 금속배선 공정을 위하여 Cu와 Si기판과의 확산을 효과적으로 방지할 확산방지막을 텅스텐(W)을 주 구성 물질로 여기에 불순물을 첨가한 W-C-N 확산방지막에 대하여 연구하였으며, 특히 W-C-N 확산방지막의 결정 및 표면 구조에 대한 물성 특성을 연구하였다. 여러 조건변화에 따라서 확산방지막의 특성을 확인하기 위하여 조건이 다르게 증착된 W-C-N 확산방지막을 상온에서 고온으로 열처리하여 열처리 전후를 WET-SPM (Scanning Probe Microscope)을 사용하여 그 물리적 특성을 조사하였다. 이러한 분석을 통하여 가장 안정된 W-C-N 확산방지막의 증착조건을 확인하였으며, 이를 기반으로 박막의 물리적 특성을 연구하였다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2009.06a
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• pp.206-207
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• 2009

PECVD를 이용하여 상온에서 Silicon nitride 박막을 제조하였다. 그리고 증착 중에 non-invasive ion energy analyzer를 이용하여 이온에너지와 이온에너지 flux룰 측정하였다. PECVD의 소스 파워는 500W, 바이어스 파워 100W으로 고정하고 주파수 250Hz으로 고정된 상태에서 펄스를 인가하여 duty ratio를 30-100%까지 변화시켰다. 작은 duty ratio 범위 (30-70%)에서 duty ratio가 감소할 때, 이온에너지와 이온에너지의 비가 감소하였다. 이 때 감소되는 굴절률은 저이온에너지 변수와 강한 연관성을 지니고 있었다. 굴절률은 1.65-2.46 사이에서 변화하였다.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.02a
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• pp.175-175
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• 2011

인체감지 적외선 센서로 사용되는 마이크로볼로미터 센서 감지재료인 $V_{2-x}W_xO_5$를 증착하고 단위소자를 제작하여 저항 및 센서성능을 측정 조사하였다. 감지재료는 $V_2O_5$에 W을 첨가하여 $V_{2-n}W_nO_5$ 타겟을 제작하였으며 RF sputtering 장비를 이용하여 $V_{1.85}W_{0.15}O_5$ 박막을 증착하였다. 증착온도 $400^{\circ}C$, $Ar/O_2$ 가스비율 50/20, 두께 200nm로 증착된 센서 재료의 특성을 조사한 결과 저항은 약 $20{\sim}70k{\Omega}$이었으며, TCR 값은 -3%/$^{\circ}C$ 이상으로 매우 우수한 박막특성을 얻었다. 볼로미터소자는 $40{\times}40{\sim}140{\times}140um^2$의 셀면적으로 설계하여 전극패턴과 습식식각공정으로 센서 구조체를 제작하였다. 소자의 성능평가는 검출기 측정장비를 이용하여 반응도 및 탐지도 특성을 조사하였다.