• 한국반도체및디스플레이장비학회:학술대회논문집
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• 한국반도체및디스플레이장비학회 2006년도 춘계학술대회
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• pp.164-167
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• 2006

In this paper, we prepared Al doped ZnO thin films by using facing targets sputtering method. Al doped ZnO thin film was deposited with different working pressure on flexible substrate. We prepared Al doped ZnO thin film at room temperature, because the flexible substrate has weak thermal resistance. From the results, we could obtain thin film with a resistivity of $8.4{\times}10^{-4}{\Omega}cm$, an average transmittance of over 80% and a film thickness of 200nm.

• 전기학회논문지
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• 제67권3호
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• pp.406-412
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• 2018

This paper describes the fabrication process of laser induced graphene (LIG) and its transfer method on to a flexible and stretchable PDMS substrate. By irradiating CO2 laser on a polyimide(PI) film surface, a localized high temperature is created, resulting in a three-dimensional porous graphene network structure with good conductivity. This LIG electrode is relatively easy to fabricate and since it is very weak the LIG electrode was transferred to a flexible PDMS substrate to increase the sturdiness as well as possible use in flexible applications. Sheet resistance, thickness, and electrochemical activity of the fabricated in-situ LIG electrodes have been examined and compared with the LIG electrodes after transferring to PDMS elastomer. The properties of the LIG electrodes were also examined depending on the $CO_2$ laser power. As the irradiated laser power increased, the LIG electrode resistance decreases and the LIG electrode thickness increased. At 4.8 W of laser power, the average sheet resistance and thickness of the fabricated LIG electrodes were approximately $31.7{\Omega}/{\Box}$ and $62.67{\mu}m$, respectively. Moreover, the electrochemical activity of the fabricated LIG electrode at 4.8 W of laser power showed a high oxidation current of $28.2{\mu}A$ after transferring to PDMS.

• 한국재료학회지
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• 제24권12호
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• pp.715-719
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• 2014

(PDDA/$SiO_2$) thin films that consisted of positively charged poly (diallyldimethylammonium chloride) (PDDA) and negatively charged $SiO_2$ nanoparticles were fabricated on a glass substrate by an applying voltage layer-by-layer (LBL) self-assembly method. In this study, the microstructure and optical properties of the (PDDA/$SiO_2$) thin films coated on glass substrate were measured as a function of the applied voltage on the Pt electrodes. When 1.0 V was applied to a Pt electrode in a PDDA and $SiO_2$ solution, the thickness of the $(PDDA/SiO_2)_{10}$ thin film increased from 79 nm to 166 nm. The surface roughness also increased from 15.21 nm to 33.25 nm because the adsorption volume of the oppositely charged PDDA and $SiO_2$ solution increased. Especially, when the voltage was applied to the Pt electrode in the $SiO_2$ solution, the thickness increase of the (PDDA/$SiO_2$) thin film was larger than that obtained when using the PDDA solution. The refractive index of the fabricated (PDDA/$SiO_2$) thin film was ca. n = 1.31~1.32. The transmittance of the glass substrate coated by (PDDA/$SiO_2$)6 thin film with a thickness of 106 nm increased from ca. 91.37 to 95.74% in the visible range.

• 한국진공학회지
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• 제9권3호
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• pp.207-215
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• 2000

진공증착 및 이온플레이팅 방법을 이용하여 냉간 압연된 강판상에 알루미늄피막을 형성시킨 후, 증발율 및 증기분포 변화를 측정하고 각 증착방법에서의 증발율에 따른 증기분포 변화를 비교 및 검토하였다. 본 실험에서의 이온플레이팅은 증발원 근처에 이온화 전극을 설치하는 방법으로 고전류 아크방전을 유도하여 $10^{-4}$ Torr 이하에서도 기존의 이온플레이팅에 비해 높은 이온화율을 얻을 수 있는 아크방전 유도형 이온플레이팅(Arc-induced ion Plating; AIIP) 방법을 이용하였다. 전자빔을 이용하면서 알루미나 크루시블을 사용하여 알루미늄을 증발시킬 경우 분당 2.0 $\mu\textrm{m}$이상의 높은 증발율을 얻을 수 있었으며, 이온플레이팅의 경우 이온화된 증기의 상호작용에 따른 산란 효과로 증발율이 다소 낮아짐을 알 수 있었다. $cos^{n/\phi}$로 이루어지는 증기분포의 결정인자(n)의 값이 진공증착의 경우는 1에 근접하는 것으로 나타났고 AIIP의 경우는 2 또는 그보다 더 큰 값으로 이루어지는 것을 확인하였다. 이로부터 이온플레이팅의 경우 이온화율 또는 기판 바이어스 전압의 효과가 다른 조건에 비해 증기분포에 더 크게 영향을 미치는 것을 확인할 수 있었다.

• 대한금속재료학회지
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• 제50권2호
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• pp.159-163
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• 2012

A TCO-less ruthenium (Ru) catalytic layer on glass substrate instead of conventional Ru/TCO/ glass substrate was assessed as counter electrode (CE) material in dye sensitized solar cells (DSSCs) by examining the effect of the Ru thickness on the DSSC performance. Ru films with different thicknesses (34, 46, 69, and 90 nm) were deposited by atomic layer deposition (ALD) on glass substrates to replace both existing catalyst and electrode layer. In order to make our comparison, we also prepared an Ru catalytic layer by a similar method on FTO/glass substrate. Finally, we prepared the $0.45cm^2$ DSSC device the properties of the DSSCs were examined by cyclic voltammetry (CV), impedance spectroscopy (EIS), and current-voltage (I-V) method. CV measurements revealed an increase in catalytic activity with increasing film thickness. The charge transfer resistance at the interface between the electrolyte and Rudecreased with increasing Ru thickness. I-V results showed that the energy conversion efficiency increased up to 1.96%. Our results imply that TCO-less Ru/glass might perform as both catalyst and electrode layer when it is used in counter electrodes in DSSCs.

• 한국자기학회지
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• 제22권1호
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• pp.6-10
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• 2012

본 연구에서는 인산 용액 하에서 2차 양극 산화 기법에 의해 제작된 양극 산화 알루미나 기판 상에 최대 13 nm 두께의 얇은 니켈 박막을 증착하며 증착 시 박막 두께에 따라 감소하는 박막의 저항 변화를 살펴보았다. 양극 산화 알루미나 막 표면에 존재하는 미세 기공 구조를 따라 증착된 니켈 박막 역시 다공 구조의 박막으로 성장하게 되며 증착된 박막의 두께 범위 내에서 박막의 저항은 $150k{\Omega}$ 이상의 값을 보이면서 박막 두께에 따른 저항의 감소가 매우 천천히 일어나는 것을 확인할 수 있었다. 측정된 저항 값은 기존에 보고된 균일한 기판 상에 증착된 동일 두께의 니켈 박막에 비해 매우 큼을 볼 수 있었으며 기판 표면에 존재하는 기공 구조에 의해 핵자가 형성될 수 있는 표면 면적 비가 박막 성장을 설명하는 스미기(percolation) 현상이론에서 예측하는 임계 값보다 매우 적어 미세 기공에 의해 박막의 성장과 함께 나타나는 전자 전도 채널의 형성이 저해됨으로 이해될 수 있다. 이와 함께 기존의 박막 두께에 따른 비저항 모델과 비교해 보았을 때 미세 기공의 경계에서 나타나는 전자 산란 현상 역시 박막저항의 증가에 기여함을 알 수 있다.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1998년도 하계학술대회 논문집 G
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• pp.2544-2546
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• 1998

The electrical and physical charateristics of Pt-Co alloy thin films on $Al_2O_3$ substrate, deposited by r.f cosputtering respectively, were analyzed with thickness of thin films ($1700{\sim}10000{\AA}$) and increasing annealing temperature ($800{\sim}1000^{\circ}C$). At input power of Pt : 4.4 W/$cm^2$, Co : 6.91 W/$cm^2$, working vacuum of 10 mTorr and annealing conditions of $1000^{\circ}C$) and 60 min, the resistivity and sheet resistivity of Pt-Co thin films with thickness of $3000{\AA}$ was $15{\mu}{\Omega}{\cdot}cm$ and 0.5 ${\Omega}/{\square}$, respectively. The TCR value of Pt-Co alloy thin films was measured with various thickness of thin films and annealing conditions. The optimum TCR value of 3850 ppm/$^{\circ}C$ in temperature range($200{\sim}400^{\circ}C$) is gained under conditions $3000{\AA}$ of thin films thickness and $1000^{\circ}C$ of annealing temperature. The thermal charateristics of Pt-Co micro heaters were analysed with Pt-Co RTD integrated on the same substrate. In the analysis of characteristics of Pt-Co micro heaters, the Pt-Co micro heaters with thickness of $3000{\AA}$ and annealing temperature of $1000^{\circ}C$ had a good linearity and temperature is up to $468.2^{\circ}C$ with 2.1 watts of the heating power.

• 한국결정성장학회지
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• 제10권2호
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• pp.100-104
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• 2000

다이아몬드 박막을 마이크로웨이브 플라즈마 방법을 이용하여 실리콘 기판위에 증착하였다. 증착된 다이아몬드 박막과 실리콘 기판의 단면을 이온 밀링 방법으로 식각한후, 경계면을 투과 전자 현미경으로 분석하였다. 다이아몬드 박막은 실리콘 기판위에 직접 성장되거나 또는 중간층이 형성된후 성장됨을 알 수 있었다. 중간층의 구성은 주로 Sic 또는 무정형 탄소로 이루어졌으며 중간층의 두께는 경계면을 따라 다르게 변하였다. 전자 회절 패턴으로부터, 경계면 주위에 잘 발달된 실리콘 기판과 다이아몬드의 결정면들이 서로 적합하게 성장되었고 있음을 알 수 있었다. 이 결과들로부터 실리콘 기판위에 성장되는 다이아몬드 박막의 초기 성장 형태를 추론할 수 있었다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.232.2-232.2
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• 2014

Since its discovery in 2004, graphene, a sp2-hybridized 2-Dimension carbon material, has drawn enormous attention. A variety of approaches have been attempted, such as epitaxial growth from silicon carbide, chemical reduction of graphene oxide and CVD. Among these approaches, the CVD process takes great attention due to its guarantee of high quality and large scale with high yield on various transition metals. After synthesis of graphene on metal substrate, the subsequent transfer process is needed to transfer graphene onto various target substrates, such as bubbling transfer, renewable epoxy transfer and wet etching transfer. However, those transfer processes are hard to control and inevitably induce defects to graphene film. Especially for wet etching transfer, the metal substrate is totally etched away, which is horrendous resources wasting, time consuming, and unsuitable for industry production. Thus, our group develops one-step process to directly grow graphene on glass substrate in plasma enhanced chemical vapor deposition (PECVD). Copper foil is used as catalyst to enhance the growth of graphene, as well as a temperature shield to provide relatively low temperature to glass substrate. The effect of growth time is reported that longer growth time will provide lower sheet resistance and higher VSG flakes. The VSG with conductivity of $800{\Omega}/sq$ and thickness of 270 nm grown on glass substrate can be obtained under 12 min growing time. The morphology is clearly showed by SEM image and Raman spectra that VSG film is composed of base layer of amorphous carbon and vertically arranged graphene flakes.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제40회 동계학술대회 초록집
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• pp.92-92
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• 2011

IZTO and ITO thin films with a thickness of 200nm were deposited on Corning glass substrate to investigate the effects of substrate temperature on their electrical and optical properties by using pulsed DC magnetron sputtering with a sintered ceramic target of IZTO (In2O3 70 wt.%, ZnO 15 wt.%, SnO2 15 wt.%) and ITO (In2O3 90 wt.%, SnO2 10 wt.%). We investigated the structural, electrical, and optical properties of IZTO and ITO films. The structural and electrical properties of both films are sensitive on the substrate temperature. As the substrate temperature is increased, the electrical resistivity of ITO films is improved, but that of IZTO film increase over than $100^{\circ}C$. All IZTO and ITO thin films have good optical properties, which showed an average of transmittance over 80%. As a result, IZTO films can be a possible material for flexible display due to the low processing temperature.