• 한국세라믹학회지
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• 제33권12호
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• pp.1353-1364
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• 1996

Recently semiconductor doped glasses have attracted attention as nonlinear optical materials because of their large third order nonlinear optical properties. The transparent and homogeneous CdS-doped SiO2 glass thin films were obtained by the dip=coating process of the sol-gel method. Thin films were consisted of glasses containing CdS microcrystallites which were formed by dissolved Cd2+ and S2- ions in a SiO2 matrix solutions. A subsequent thermal treatment of this samples led the formation of colloidal agglomerates and finally of microcrystallites. The size of CdS microcrystallites was about 4 to 15 nm after thermal treatments at various heating conditions. From the optical absorption spectra of the CdS-doped SiO2 glass films it was found that the absorption edge was blue-shifted compared with that of the bulk CdS crystal(~2, 4 eV) and that the amount of energy shift was inversely proportional to the crystal size. And the band gap energy increased with the decrease in crystallite size indicating that the quantum size effects occured.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제40회 동계학술대회 초록집
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• pp.442-442
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• 2011

Electronic and magnetic properties of bilayer zigzag graphene nanoribbon (bZGNR) are studied using pseudopotential density functional method. The edge atoms in the top and bottom layers of bZGNR make a weak hybridization, which leads to electronic structures different from monolayer ZGNR. For asymmetric bZGNR, where the top and bottom layers have different widths, one edge is pinched by the interlayer bonding and the other sustains antiferromagnetic ordering. A small amount of charge transfer occurs from narrower to wider layer, producing spin-polarized electron and hole pockets. External electric field produces asymmetric energy-gap opening for each spin component, inducing half-metallicity in bZGNR.

• 세라미스트
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• 제22권1호
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• pp.27-35
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• 2019

Research on ultraviolet (UV) light detection has attracted considerable attention from scientific researchers in related fields. It can be said that it is a very important time to accurately monitor the UV irradiation amount according to the wavelength region in real time. The oxide is very diverse in its kind and has the advantage of being able to efficiently control the band gap through band gap engineering. In addition, it is very stable in response to heat and atmospheric oxygen when UV is absorbed. Also, there is a known method that can effectively manufacture oxide nanoparticles and nanorods through various synthesis methods, and researches for improving the sensitivity of UV sensors have been carried out using this method. In this paper, we introduce the materials that can be used as UV sensors among various wide band oxide materials, and review the results of researches of various UV sensors using nano materials.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2006년도 제37회 하계학술대회 논문집 B
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• pp.1087-1088
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• 2006

In this paper, the inductive power collector using electromagnetic Induction for vehicle such as the PRT(Personal Rapid Transit) system is suggested and some ideas for power collector design to improve the power transfer performance are presented. The inductive power of secondary part is related to amount of linked flux to secondary part by the length of air-gap, which is expected by such a system parameter as mutual inductance. This paper will study for the transfer characteristic of power from input to output and equation including mutual inductance.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2007년도 하계학술대회 논문집 Vol.8
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• pp.66-67
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• 2007

We have developed reflective information display using opposite-charged two particles. An appropriate amount of both the yellow and the black powers are putted between the ITO patterned glass substrate separated with cell gap. The rib maintains the cell gap and prevents the interference between the pixels. When a negative voltage is applied to the upper ITO electrode, the positively charged black powder moves to the upper electrode viewing a black appearance. In case of positive voltage is applied to this electrode white particle is observed. So we analyzed the electrical and optical properties of our charged particle type display panel.

• 한국수자원학회논문집
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• 제53권10호
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• pp.889-902
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• 2020

본 연구에서는 GLDAS (Global Land Data Assimilation System)와 GLEAM (Global Land Evaporation Amsterdam Model) 증발산량의 적정성을 평가하기 위해 설마천 유역에서 관측된 에디공분산 기반의 잠열 플럭스를 검증자료로 활용하였다. 잠열 플럭스로부터 증발산량을 산정하기 위해 Koflux 프로그램으로 자료처리하였으며, 자료처리 후 발생된 빈구간을 보충(Gap-filling)하기 위해 FAO-PM (Food and Agriculture Organization-Penman Monteith), 평균 일변동(Mean Diurnal Variation, MDV), 칼만 필터(Kalman Filter)의 3가지 방법으로 대체 증발산량을 산정하였다. 본 연구에서는 3가지 방법 중 칼만 필터(Kalman Filter) 기반의 증발산량이 우수한 Bias와 RMSE를 보여 자료보충 방법으로 채택하였다. 공간증발산량은 GLDAS의 경우 Noah (version 2.1, 3시간, 공간해상도 0.25°)로 추출하였으며 GLEAM의 경우는 GLEAM(version 3.1a, 1일, 공간해상도 0.25°)를 이용하였다. GLDAS와 GLEAM의 공간증발산량을 에디공분산 기반의 증발산량으로 적정성을 평가한 결과, GLDAS의 증발산량이 에디공분산 기반과 비교적 적정한 결과를 나타내었다.

• 대한환경공학회지
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• 제31권1호
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• pp.29-34
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• 2009

표면처리폐수 내 질산성 질소를 제거하기 위한 전기화학적 처리공정에서 전극간격, 환원제, 1단 처리수 반송, 타 물질과 동시 처리 등 네 가지 조건을 변화시키며 실험을 진행하였다. 실험 결과, 전극간격은 10 mm일 때 질산성 질소 제거효율이 높았으며 10 mm 보다 전극간격이 좁아질 경우 농도분극 현상의 증가로 인해 제거효율이 감소하며 10 mm 보다 넓어질 경우 전압이 상승하여 에너지 소모가 증가하였다. 환원제 영향에 대한 실험 결과, 질산성 질소가 환원되는 과정에서 수소가 소모되기 때문에 수소이온 농도가 높은 산성조건에서 더 원활한 환원반응이 이루어졌으며 아연을 1.2배 투입할 경우 질산성 질소와의 반응량이 증가하여 질산성 질소 제거효율이 증가하였다. 1단 처리수를 반송할 경우 난류가 형성되어 환원전극에 부착된 아연이 탈착되어 재 이용되고 내부 확산이 증가하여 농도분극현상이 감소함으로 인해 질산성 질소 제거효율이 증가하였으며 아연 투입량 감소 효과가 나타났다. 암모니아성 질소는 질산성 질소 제거에 영향을 미치지 않았고 폐수 내 염소성분이 충분할 경우 질산성 질소와 동시 처리에도 문제가 없는 것으로 나타났다. 중금속은 환원되는 과정에서 전자를 소모하여 질산성 질소 제거효율은 감소하지만 전류밀도 증가나 본 장치의 전단을 중금속 제거용으로 사용하는 방법 등으로 해결이 가능할 것으로 생각한다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제40회 동계학술대회 초록집
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• pp.53-53
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• 2011

As the dimension of Cu interconnects has continued to reduce, its resistivity is expected to increase at the nanoscale due to increased surface and grain boundary scattering of electrons. To suppress increase of the resistivity in nanoscale interconnects, alloying Cu with other metal elements such as Al, Mn, and Ag is being considered to increase the mean free path of the drifting electrons. The formation of Al alloy with a slight amount of Cu broadly studied in the past. The study of Cu alloy including a very small Al fraction, by contrast, recently began. The formation of Cu-Al alloy is limited in wet chemical bath and was mainly conducted for fundamental studies by sputtering or evaporation system. However, these deposition methods have a limitation in production environment due to poor step coverage in nanoscale Cu metallization. In this work, gap-filling of Cu-Al alloy was conducted by cyclic MOCVD (metal organic chemical vapor deposition), followed by thermal annealing for alloying, which prevented an unwanted chemical reaction between Cu and Al precursors. To achieve filling the Cu-Al alloy into sub-100nm trench without overhang and void formation, furthermore, hydrogen plasma pretreatment of the trench pattern with Ru barrier layer was conducted in order to suppress of Cu nucleation and growth near the entrance area of the nano-scale trench by minimizing adsorption of metal precursors. As a result, superconformal gap-fill of Cu-Al alloy could be achieved successfully in the high aspect ration nanoscale trenches. Examined morphology, microstructure, chemical composition, and electrical properties of superfilled Cu-Al alloy will be discussed in detail.

• 에너지공학
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• 제1권1호
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• pp.66-75
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• 1992

이중창의 열전달 성능을 수치해석과 실험적 방법을 통하여 조사하였다. 이중창 사이의 간격이 0.5cm에서 10cm사이의 실제적인 범위에서 이중창 사이의 간격이 작을 때에는 전도에 의한 열전달이 두드러졌으며 이중창 사이의 간격이 넓어지고 Rayleigh 수가 높은 영역에서는 대류에 의한 열전달이 크게 나타나 이중창 간격이 넓어진 이점을 크게 상쇄시켰다. 이와 같은 이중창 단열문제에 대한 보완책으로 이중창 중앙에 하나의 유리창을 더 설치한 3중창 경우에 대해 대류열전달 감소효과와 복사열차폐(radiation shield) 효과를 검토하였으며 또한 이중창 중간 높이에 스페이서(spacer)를 설치하여 대류유동 강도를 줄이는 방안 등에 대한 분석이 이루어졌다. 3중창을 사용한 경우에는 이중창에 비해 30-50%, 이중창에 스페이서를 설치한 경우에는 l0% 정도의 에너지 절약 효과를 기대할 수 있다.

• 설비공학논문집
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• 제18권3호
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• pp.254-261
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• 2006

The effect of enhanced geometry (pore diameter, gap width) is investigated on the pool boiling of R-123/oil mixture for the enhanced tubes having pores with connecting gaps. Tubes with different pore diameters (and corresponding gap widths) are specially made. Significant heat transfer degradation by oil is observed for the present enhanced tubes. At 5% oil concentration, the degradation is 26 to 49% for $T_{sat}=4.4^{\circ}C$. The degradation increases 50 to 67% for $T_{sat}=26.7^{\circ}C$. The heat transfer degradation is significant even with small amount of oil (20 to 38% degradation at 1% oil concentration for $T_{sat}=4.4^{\circ}C$), probably due to the accumulation of oil in sub-tunnels. The pore size (or gap width) has a significant effect on the heat transfer degradation. The maximum degradation is observed for $d_p$ = 0.20 mm tube at $T_{sat}=4.4^{\circ}C$, and for $d_p$=0.23 mm tube at $T_{sat}=26.7^{\circ}C$. The minimum degradation is observed for $d_p$=0.27 mm tube for both saturation temperatures. It appears that the oil removal is facilitated for the larger pore diameter (along with larger gap) tube. The highest heat transfer coefficient with oil is obtained for $d_p$ =0.23 mm tube, which yielded the highest heat transfer coefficient for pure R-123. The heat transfer degradation increases as the heat flux decreases.