• 대한전기학회:학술대회논문집
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• 대한전기학회 2003년도 하계학술대회 논문집 C
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• pp.1917-1919
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• 2003

본 연구에서는 바이오 및 환경 분야에 적용 가능한 미세 유체소자 제작에 있어서 4" 유리 / 유리 웨이퍼접합을 시도하였으며, 접합결과 90%이상의 접합면적을 보였다. 접합된 샘플을 산 및 알카리 조건에 따른 인장시험결과 모든 조건에서 약 $2kgf/mm^2$ 이상의 접합강도를 보였으며 파괴는 접합면이 아닌 모재에서 발생되었다. 또한 미세유체소자 제작에 있어서 초음파를 이용하여 유리를 가공하였으며, 폭 $300{\mu}m$, 깊이 $200{\mu}m$의 미세채널을 제작하였다.

• 산업식품공학
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• 제14권1호
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• pp.21-26
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• 2010

C-Reactive protein (CRP), which is an 118 kDa pentameric protein, was secreted by the liver is an important biomarker for coronary disease, hypertension and inflammation. In this study, a method for CRP detection exploiting quantum dot (Qdot)-antibody conjugate was developed according to an indirect-competitive immunosensing protocol. For this purpose, a streptavidin-bound $Qdot_{605}$ was linked with a separately prepared biotinylated monoclonal antirat CRP antibody to produce a Qdot-antibody conjugate. The immunosensing was performed at 0.1 and 20 nM of the coating antigen and conjugate, respectively. The current method was found very sensitive in CRP detection, judging from the concentration-dependent fluorescence emission.

• 센서학회지
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• 제10권5호
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• pp.292-303
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• 2001

본 연구에서는 수평형 전계 방출 소자를 제작하고 그 특성을 측정하였다. 이를 진공자장 센서에 이용하기 위하여 Lorentz 원리를 응용하여 센서를 설계하고 제작하였다. $POCl_3(10^{20}cm^{-3})$ 도핑된 다결정 실리콘을 전계 방출 소자의 음극 및 양극 재료로 이용하였으며 그 두께는 각각 $2\;{\mu}m$였다. PSG(두께 $2\;{\mu}m$)를 희생층으로 사용하여 최종 단계에서 불산을 이용하여 제거하고 승화건조법을 이용하여 소자의 기판 점착 현상을 방지하였다. 제작된 소자를 유리기판 #1 위에 silver paste로 고정시키고 Cr 전극 패드와 와이어본딩 한 뒤 진공내에서 양극접합공정을 이용하여 소자를 $1.0{\times}10^{-6}\;Torr$에서 진공 실장하였다. 실장 후 게터를 활성화하여 내부진공도를 향상시켰다. 이렇게 패키징된 소자는 두달여 기간 동안 특별한 특성저하 없이 잘 동작되었으며 그 이상의 기간에 대해서는 확인하지 못하였다. 패키징된 자장 센서는 패키징하기 전 진공챔버 내에서 보인 특성치와 별다른 차이 없이 잘 동작되었으며 단지 약간의 전류 감소 현상만이 관찰되었다. 측정된 센서의 감도는 약 3%/T로서 작은 값이었으나 그 가능성을 확인할 수는 있었다.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2012년도 추계학술대회 논문집
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• pp.89-90
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• 2012

• 한국정보디스플레이학회:학술대회논문집
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• 한국정보디스플레이학회 2006년도 6th International Meeting on Information Display
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• pp.125-125
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• 2006

We present a low temperature thermal process for the transparent dielectric layer, barrier rib, and white back dielectric layer on the soda-lime glass substrate of the PDP by the $TruNano^{TM}$ processor in combination with a compositional modification to the conventional dielectric pastes. By this method the firing temperature can be lowered by more than $100^{\circ}C$.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2010년도 하계학술대회 논문집
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• pp.180-180
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• 2010

본 연구에서는 P-Type의 NiO를 Glass기판의 ITO전극위에 RF-스퍼터링 방법으로 증착하였으며, NiO 완충층의 두께 변화에 따른 OLED (Organic Light Emitting Diode) 소자의 발광 특성에 대해 연구하였다[1, 2]. NiO는 우수한 전기 광학적 특성을 가지고 있어 OLED소자의 구동전압, 발광 효율 등의 특성을 향상 시킬 수 있다[3]. NiO 완충층의 두께 변화는 스퍼터링 증착시간을 통해 5-20 nm로 조절하였으며 소자의 구조는 Glass/ITO/NiO(0~20nm)/NPB(40nm)/Alq3(60nm)/LiF(0.5nm)/Al(120nm)형태로 제작하였다. ITO/NPB 계면에 NiO 완충층을 삽입함으로써 OLED 발광소자의 구동전압을 ~8V에서 ~5V (NiO, 10nm)로 낮출 수 있었다.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2008년도 Techno-Fair 및 추계학술대회 논문집 전기물성,응용부문
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• pp.131-132
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• 2008

We describe a fabrication method of submicron glass trenches which have embedded metal lines for the future application of nano-scale RF MEMS devices. The glass wafer was etched using two different conditions to identify the relationship between the slope of glass trenches and the slope of photroresist. A self-aligned metal photomask and negative photroresist (PR) slope were used to insert metal lines inside the glass trenches. The PR slope patterned by backside photolithography was affected by the profile of preformed glass trenches. Gold was well fabricated in the $0.7{\mu}m$ wide trench thanks to the negative PR slope. Nano-scale glass trenches with embedded metal lines can be used as a bottom electrode in submicron beam resonators operating with a high resonant frequency.

• 한국전기전자재료학회논문지
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• 제34권2호
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• pp.110-114
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• 2021

In this study, we fabricated light-weight solar module for various applications such as building integrated photovoltaics (BIPV), vehicles, trains, etc. Ethylene tetra fluoro ethylene (ETFE) film was applied as a material to replace the cover glass, which occupies more than 65% of the weight of the PV module. Glass fiber reinforced plastic (GRP) was applied to the ones with a low durability by replacing the cover glass to ETFE. Moreover, to achieve a high solar power conversion in this study, we applied a shingled design to weight reduced solar modules. The shingled module with GRP shows 183.7 W of solar-to-power conversion, and the output reduction rate after weight load test was 1.14%.

• 한국분말야금학회:학술대회논문집
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• 한국분말야금학회 2004년도 International Symposium on Powder Materials and Processing
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• pp.100-101
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• 2004

• 한국재료학회지
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• 제22권2호
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• pp.61-65
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• 2012

A $Li_2O-2SiO_2$ ($LS_2$) glass was investigated as a lithium-ion conducting oxide glass, which is applicable to a fast ionic conductor even at low temperature due to its high mechanical strength and chemical stability. The $Li_2O-2SiO_2$ glass is likely to be broken into small pieces when quenched; thus, it is difficult to fabricate a specifically sized sample. The production of properly sized glass samples is necessary for device applications. In this study, we applied spark plasma sintering (SPS) to fabricate $LS_2$ glass samples which have a particular size as well as high transparency. The sintered samples, $15mm\phi{\times}2mmT$ in size, ($LS_2$-s) were produced by SPS between $480^{\circ}C$ and $500^{\circ}C$ at 45MPa for 3~5mim, after which the thermal and dielectric properties of the $LS_2$-s samples were compared with those of quenched glass ($LS_2$-q) samples. Thermal behavior, crystalline structure, and electrical conductivity of both samples were analyzed by differential scanning calorimetry (DSC), X-ray diffraction (XRD) and an impedance/gain-phase analyzer, respectively. The results showed that the $LS_2$-s had an amorphous structure, like the $LS_2$-q sample, and that both samples took on the lithium disilicate structure after the heat treatment at $800^{\circ}C$. We observed similar dielectric peaks in both of the samples between room temperature and $700^{\circ}C$. The DC activation energies of the $LS_2$-q and $LS_2$-s samples were $0.48{\pm}0.05eV$ and $0.66{\pm}0.04eV$, while the AC activation energies were $0.48{\pm}0.05eV$ and $0.68{\pm}0.04eV$, respectively.