• 한국식품과학회지
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• 제48권2호
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• pp.122-127
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• 2016

아사이베리의 특징적인 향기성분을 동정하기 위하여 SAFE와 LLCE를 이용하여 추출하고 GC-MS와 GC-O로 분석하였다. 아사이베리에서 공통적으로 동정된 휘발성 향기성분은 2-phenylethanol, (Z)-3-hexenol과 benzyl alcohol 등으로 함량이 높았으며 8-hydroxy linalool과 maltol은 LLCE에서 높은 함량을 나타내었다. 아사이베리의 휘발성 향기성분은 알코올류가 가장 함량이 높았으며 아사이베리의 중요한 휘발성 향기성분이라고 생각된다. 아사이베리의 향 활성 화합물 중 ${\beta}-damascenone$은 SAFE에서 $log_2FD=4$와 LLCE에서 $log_2FD=1$을 나타냈으며 장미향과 베리향 특성을 나타내어 아사이베리의 특징적인 향에 기여하는 중요한 화합물이라 생각된다. 또한 trans-linalool oxide, (Z)-3-hexenol과 2-phenylethanol 등이 아사이베리의 향 활성 화합물로 동정되었다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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• pp.197.2-197.2
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• 2015

Low-cost, high efficiency solar cells are tremendous interests for the realization of a renewable and clean energy source. ZnTe based solar cells have a possibility of high efficiency with formation of an intermediated energy band structure by impurity doping. In this work, the ZnTe:O/CdS/ZnO structure was fabricated by pulsed laser deposition (PLD) technique. A pulsed (10 Hz) Nd:YAG laser operating at a wavelength of 266 nm was used to produce a plasma plume from an ablated a ZnTe target, whose density of laser energy was 4.5 J/cm2. The base pressure of the chamber was kept at a pressure of approximately $4{\times}10-7Torr$. ZnO thin film with thickness of 100 nm was grown on to ITO/glass, and then CdS and ZnTe:O thin film were grown on ZnO thin film. Thickness of CdS and ZnTe:O were 50 nm and 500 nm, respectively. During deposition of ZnTe:O films, O2 gas was introduced from 1 to 20 mTorr. For fabricating ZnTe:O/CdS/ZnO solar cells, Au metal was deposited on the ITO film and ZnTe:O by thermal evaporation method. From the fabricated ZnTe:O/CdS/ZnO solar cell, current-voltage characteristics was measured by using HP 4156-a semiconductor parameter analyzer. Finally, solar cell performance was measured using an Air Mass 1.5 Global (AM 1.5 G) solar simulator with an irradiation intensity of 100 mW cm-2.

• 한국광학회:학술대회논문집
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• 한국광학회 2009년도 동계학술발표회 논문집
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• pp.133-134
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• 2009

Cold temperature development (CTD) of electron beam (EB) patterned resists and subsequent dry etching were investigated for fabrication of nano-patterned Niobium (Nb). Bulky Nb fims on GaAs substrates were deposited with EB evaporation. Line patterns on Nb cathode were fabricated by EB patterning and reactive ion etching (RIE). Size deviations of nano-sized line patterns from CAD designed patterns are dependent on the EB total exposure, but it can be improved by CTD of EB-exposed resist. Line patterns of 10 to 300 nm widths of EB-exposed resist patterns were drawn under various exposure conditions of $0.2{\mu}s$/dot (total 240,000 dot) with a constant current (50 pA). Compared with room temperature development (RTD), the CTD improves pattern resolution due to the suppression of backscattering effect. RIE with $CF_4$ was performed for formation of several nano-sized line patterns on Nb. Each EB-resist patterned samples with RTDs and CTDs were etched with two different $CF_4$ gas pressures of 5 Pa. Nb etching rate increases while GaAs (or ZEP) etching rate decreases as the chamber pressure increases. This different dependent of the etching rate on the $CF_4$ pressure between Nb and GaAs (or ZEP) has a significant meaning because selective etching of nano-sized Nb line patterns is possible without etching of the underlying active layer.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2002년도 춘계학술대회 논문집 센서 박막재료 반도체재료 기술교육
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• pp.55-61
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• 2002

Ultra-fine particles of $SnO_{2}$ was synthersized by the sol-gel powder processing using tin(II) chloride dihydrate$(SnCl_{2}{\cdot}2H_{2}O)$ and ethanol$(C_{2}H_{5}OH)$ as raw materials. Gel powders can be obtained by drying of sol at $120^{\circ}C$ after aging 72hrs and 168hrs. The amount of $SnO_{2}$ phase was increased with temperature because of the evaporation of volatile components, and the creation of $SnO_{2}$ phase was almost done by the heat treatment at $700^{\circ}C/30min$ The grain sizes after firing are about 20-30nm, and it showed the narrow distribution of grain size. The specimens to measure electrical properties were fabricated by the thick film screen printing technique on the alumina substrates. The conductance of $SnO_{2}$ was increased with temperature up to $380^{\circ}C$ by the typical conduction mechanism of semiconducting ceramics. There was a region of constant conductance between about $200^{\circ}C$ and $380^{\circ}C$ due to the increment of electron concentration with temperature and the annihilation of conduction carriers by the absorption and electron trapped-ionization of oxygen on the surface of $SnO_{2}$, It was finally showed the intrinsic behaviors above $450^{\circ}C$. The sensing properties of response time, recovery, and sensitivity of CO were improved with aging time.

• 한국컴퓨터산업학회논문지
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• 제8권1호
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• pp.49-56
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• 2007

빔의 열적효과는 세포조직의 서로 다른 구성성분과 레이저 빔의 서로 다른 파장에서 다른결과를 나타내며 세포조직에서 온도증가는 먼저 응고가 이루어지고, 절단이나 탄화과정이 일어나며 $300^{\circ}$이상에서는 세포조직의 파괴에 의한 증발이 발생하게 된다. $CO_2$ 레이저는 최소한 조직손상으로 이러한 효과를 얻는데 최적이라고 보며 0.1mm의 최소한의 세포조직 깊이에서 일어나는 효과의 근본적인 장점은 생체조직이나 내장기관에 안정적이다. $CO_2$레이저사용에 있어서 단점은 무엇보다도 세포파괴에서 생성되는 입자들의 부품흡착 등으로 결과적으로 레이저의 출력감소가 일어나는데, 영 전압, 영 전류 스위칭 포워드 컨버터를 도입하여 기존의 하드 스위칭 포워드 컨버터에 있어서 Turn-off, on시 발생되는 스위칭 방식을, 적용함으로써 1차 측 스위칭 소자의 Turn-off, on시 영전압, 영전류 스위칭을 이루어 정밀도가 요구되는 산부인과용 $CO_2$ 연속 형 레이저의 고압출력 모듈에 따른 펄스 트랜스의 안정화에 필수적으로 기여하며, 레이저 출력과 안정화가 되도록 설계 및 제작한 결과, 기존제품보다 향상된 결과를 가져왔다. 추후 시스템적으로 보완을 하면 우수한 결과가 될 것으로 사려된다.

• 한국수소및신에너지학회논문집
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• 제28권4호
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• pp.401-406
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• 2017

When Liquified Natural Gas (LNG) is vaporized into NG for industrial and household usage, tremendous cold energy was transferred from LNG to seawater during phase-changing process. This heat exchanger loop is not only a waste of huge cold energy, but will cause thermal pollution to the coastal fishery area also when cold water was re-injected into the sea. In this study, an innovation design has been performed to reclaim the cold energy for -35 to $62^{\circ}C$ refrigerated warehouse. Conventionally, this was done by installing mechanical refrigeration systems, necessitating tremendous electrical power to drive temperature. A closed loop LNG heat exchangers in series was designed to replace the mechanical or vapor-compression refrigeration cycle by process simulator. The process simulation software of PRO II with provision has been used to simulate this process for various conditions, what to effect on cold energy and used energy for re-liquefaction and evaporation process. In addition, through analysis the effect of the change of LNG supply pressure on sensible and latent heat, optimum operational conditions was suggested for LNG cold energy warehouse.

• 한국재료학회:학술대회논문집
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• 한국재료학회 2011년도 추계학술발표대회
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• pp.17.2-17.2
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• 2011

Double-walled carbon nanotubes (DWCNTs) were grown with vertical alignment on a Si wafer by using catalytic thermal chemical vapor deposition. This study investigated the effect of pre-annealing time of catalyst on the types of CNTs grown on the substrate. The catalyst layer is usually evolved into discretely distributed nanoparticles during the annealing and initial growth of CNTs. The 0.5-nm-thick Fe served as a catalyst, underneath which Al was coated as a catalyst support as well as a diffusion barrier on the Si substrate. Both the catalyst and support layers were coated by using thermal evaporation. CNTs were synthesized for 10 min by flowing 60 sccm of Ar and 60 sccm of H2 as a carrier gas and 20 sccm of C2H2 as a feedstock at 95 torr and $750^{\circ}C$. In this study, the catalyst and support layers were subject to annealing for 0~420 sec. As-grown CNTs were characterized by using field emission scanning electron microscopy, high resolution transmission electron microscopy, Raman spectroscopy, and atomic force microscopy. The annealing for 90~300 sec caused the growth of DWCNTs as high as ~670 ${\mu}m$ for 10 min while below 90 sec and over 420 sec 300~830 ${\mu}m$-thick triple and multiwalled CNTs occurred, respectively. Several radial breathing mode (RBM) peaks in the Raman spectra were observed at the Raman shifts of 112~191 cm-1, implying the presence of DWCNTs, TWCNTs, MWCNTs with the tube diameters 3.4, 4.0, 6.5 nm, respectively. The maximum ratio of DWCNTs was observed to be ~85% at the annealing time of 180 sec. The Raman spectra of the as-grown DWCNTs showed low G/D peak intensity ratios, indicating their low defect concentrations. As increasing the annealing time, the catalyst layer seemed to be granulated, and then grown to particles with larger sizes but fewer numbers by Ostwald ripening.

• 한국신재생에너지학회:학술대회논문집
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• 한국신재생에너지학회 2007년도 춘계학술대회
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• pp.250-253
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• 2007

An evaporated Ti/Pd/Ag contact system is most widely used to make high-efficiency silicon solar cells, however, the system is not cost effective due to expensive materials and vacuum techniques. Commercial solar cells with screen-printed contacts formed by using Ag paste suffer from a low fill factor and a high shading loss because of high contact resistance and low aspect ratio. Low-cost Ni and Cu metal contacts have been formed by using electroless plating and electroplating techniques to replace the Ti/Pd/Ag and screen-printed Ag contacts. Ni/Cu alloy is plated on a silicon substrate by electro-deposition of the alloy from an acetate electrolyte solution, and nickel-silicide formation at the interface between the silicon and the nickel enhances stability and reduces the contact resistance. It was, therefore, found that nickel-silicide was suitable for high-efficiency solar cell applications. The Ni contact was formed on the front grid pattern by electroless plating followed by anneal ing at $380{\sim}400^{\circ}C$ for $15{\sim}30$ min at $N_{2}$ gas to allow formation of a nickel-silicide in a tube furnace or a rapid thermal processing(RTP) chamber because nickel is transformed to NiSi at $380{\sim}400^{\circ}C$. The Ni plating solution is composed of a mixture of $NiCl_{2}$ as a main nickel source. Cu was electroplated on the Ni layer by using a light induced plating method. The Cu electroplating solution was made up of a commercially available acid sulfate bath and additives to reduce the stress of the copper layer. The Ni/Cu contact was found to be well suited for high-efficiency solar cells and was successfully formed by using electroless plating and electroplating, which are more cost effective than vacuum evaporation. In this paper, we investigated low-cost Ni/Cu contact formation by electroless and electroplating for crystalline silicon solar cells.

• 한국진공학회지
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• 제18권6호
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• pp.453-458
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• 2009

SiOC 박막을 BTMSM과 산소의 혼합가스를 사용하여 CVD 방법으로 증착하였다. 박막의 특성은 가스 유량비에 따라서 변하였다. 유전상수는 MIS 구조를 이용하여 C-V 측정법에 의하여 얻었다. 결합의 말단을 구성하는 Si-$CH_3$ 결합 사이의 공간효과에 의해서 기공이 만들어지며, 기공의 형성에 의해서 박막의 두께가 증가하였다. 그러나 분극의 감소에 의해서 만들어지는 SiOC 박막은 두께가 감소하면서 유전상수도 감소되었다. 열처리 후 유전상수는 수산기의 기화에 의해서 감소되었다. 박막의 두께는 분극의 감소에 의한 유전상수의 감소와 연관이 있었다. 굴절률은 박막의 두께에 반비례하는 경향성이 있으며, 박막의 두께와 굴절률의 경향성은 열처리 후에도 변하지 않았다.

• 한국재료학회:학술대회논문집
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• 한국재료학회 2011년도 춘계학술발표대회
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• pp.47.2-47.2
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• 2011

광전환 효율 20% (AM1.5G) 이상의 고효율 화합물 박막태양전지의 광흡수층으로 많은 관심을 받고 있는 $Cu(In,Ga)Se_2$ (CIGS) 태양전지의 광흡수층은 다양한 공정에 의해 제조가 가능하다. 현재 고효율 CIGS 셀 생성을 위해 널리 사용되고 있는 CIGS 흡수층 성장공정은 "co-evaporation (동시증발법)"과 2-step 공정이라 불리는 "precursorselenization(전구체-셀렌화)" 방법이다. 동시증발법은 개별원소 Cu, In, Ga, Se들을 고진공 분위기에서 고온(550~600$^{\circ}C$) 기판위에 증착하는 방법으로 소면적에서 가장 좋은 효율(~20%)을 보이는 공정이다. 하지만, 고온, 고진공 공정조건과 대면적 증착시 온도 및 조성 불균일 등의 문제점 등으로 상용화에 어려움이 있다. 전구체-셀렌화 공정은 1단계에서 다양한 방식(예: 스퍼터링, 전기도금, 프린팅 등) 방식으로 CuGaIn 전구체를 증착하고, 2단계에서 고온(550~600$^{\circ}C$)하에 H2Se gas 혹은 Se vapor와 반응시켜 CIGS를 생성한다. 일본의 Showa Shell와 Honda Soltec 등에 의해 이미 상업화 되었듯이, 저비용 대면적으로 상업화 가능성이 높은 공정으로 평가되고 있다. 하지만, 2단계에서 사용되는 H2Se 및 Se vapor의 유독성, 기상 Se과 금속전구체 간의 느린 셀렌화 반응속도, 셀렌화반응 후 생성된 CIGS 박막 두께방향으로의 Ga 불균일 분포, 생성된 CIGS/Mo 계면 접착력 저하 등의 문제점들이 개선, 해결되어야만 상업화에 성공할 수 있을 것이다. 본 연구에서는 Se layer가 코팅된 금속전구체의 셀렌화 반응메카니즘을 in-situ high-temperature XRD를 이용하여 연구하였다. 금속전구체는 스퍼터링, 스프레이 등 다양한 방법으로 제조되었고, 반응메카니즘 연구결과를 바탕으로 Se 코팅된 금속전구체를 이용한 급속열처리 공정의 최적화를 시도하였다.