• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1995년도 춘계학술대회 논문집
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• pp.58-61
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• 1995

레이저 유기에 대한 GaAs 의 건석에칭에 있어서 기존의 $CCl_4$와CCl$_2$F$_2$ 가스를 에칭하스로 사용하는 대신에 본 연구팀이 새로 개발한 CFCs 대체가스를 사용하여 기존의 가스와의 에칭률과 그 가공된 형태를 비교하였다. 실험은 power 밀도 12.7 MW/$\textrm{cm}^2$에서 27 MW/$\textrm{cm}^2$까지로 가변시키면서 하고 에칭가스의 압력은 260 Torr에서760 Torr 까지 변화를 주면서 하였다. 빔의 주사속도는 8.3$\mu\textrm{m}$/sec에서 80$\mu\textrm{m}$/sec 까지 가변을 시켰다. 그 결과 CHCiF$_2$가스에서의 에칭율(etch rate)은 최대 136$\mu\textrm{m}$/sec이고 aspect ratio 는 2.6 이 됨을 알 수 있었다. 애칭된 형태를 측정하기 위해서 SEM(Scanning Electron Microscopy)을 사용하였으며, 시료 표면의 물질 분석을 위해서 AES(Auger Electron Spectroscopy)를 사용하였다.

• 한국결정성장학회지
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• 제9권1호
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• pp.89-93
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• 1999

나노 구조를 갖는 다공질 규소의 표면과 투명하고 전도성을 갖는 접촉방법을 얻기 위해 다공질 규소 표면에 CdTe 화합물 박막을 전착시키는 방법을 시도하였다. CdTe 화합물 박막은 1 M의 $CdSO_4$와 1mM의 $TeO_4$가 혼합된 전해액 속에서 전착 전위 2-2.3V(vs. Ag/AgCl)로 다공질규소의 표면에 전착시켰다. X선 회절 측정결과 다공질규소 표면에 CdTe 화합물 박막이 생성되었음이 확인되었고, AES 분석결과 표면에서 약 80nm 깊이까지 Cd 및 Te 원소가 균일하게 존재하였다. 그리고 CdTe 화합물 박막이 전착된 다공질규소의 PL 특성은 발광의 세기는 약간 검소하였고 최대파장값은 고에너지 쪽으로 이동하였다. 이 결과로 보아 CdTe 전착 박막이 나노 구조를 갖는 다공질규소와 투명하고 전도성을 갖는 접촉물질로 이용될 수 있음이 밝혀졌다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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• pp.119-119
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• 2015

Ion beam sputtering has been widely used in Secondary Ion Mass Spectrometry (SIMS), X-ray Photoelectron Spectroscopy (XPS), and Auger Electron Spectroscopy (AES) for depth profile or surface cleaning. However, mainly due to severe matrix effects such as surface composition change from its original composition and damage of the surface generated by ion beam bombardment, conventional sputtering skills using mono-atomic primary ions with energy ranging from a few hundred to a thousand volts are not sufficient for the practical surface analysis of next-generation organic/inorganic device materials characterization. Therefore, minimization of the surface matrix effects caused by the ion beam sputtering is one of the key factors in surface analysis. In this work, the electronic structure of a $Ta_2O_5$ thin film on $SiO_2/Si$ (100) after Ar Gas Cluster Ion Beam (GCIB) sputtering was investigated using X-ray photoemission spectroscopy and compared with those obtained via mono-atomic Ar ion beam sputtering. The Ar ion sputtering had a great deal of influence on the electronic structure of the oxide thin film. Ar GCIB sputtering without sample rotation also affected the electronic structure of the oxide thin film. However, Ar GCIB sputtering during sample rotation did not exhibit any significant transition of the electronic structure of the $Ta_2O_5$ thin films. Our results showed that Ar GCIB can be useful for potential applications of oxide materials with sample rotation.

• 전기학회논문지
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• 제60권6호
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• pp.1169-1174
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• 2011

CdTe thin-film solar cell technology is well known that it can theoretically improve its conversion efficiency and manufacturing costs compared to the conventional silicon solar cell technology, due to its optical band gap energy (about 1.45eV) for solar energy absorption, high light absorption capability and low cost requirements for producing solar cells. Although the prior studies obtained the high light absorption, CdTe thin film solar cell has not been come up to the sufficient efficiency yet. So, doping method was selected for the improvement of the electrical characteristics in CdTe solar cells. Some elements including Cu, Ag, Cd and Te were generally used for the p-dopant as substitutional acceptors in CdTe thin film. In this study, the sputtering-deposited CdTe thin film was immersed in $AgNO_3$ solution for ion exchange method to dope Ag ions. The effects of immersion temperature and Ag-concentration were investigated on the optical properties and electrical characteristics of CdTe thin film by using Auger electron spectroscopy depth-profile, UV-visible spectrophotometer, and a Hall effect measurement system. The best optical and electrical characteristics were sucessfully obtained by Ag doping at high temperature and concentration. The larger and more uniform diffusion of Ag ions made increase of the Ag ion density in CdTe thin film to decrease the series resistance as well as mede the faster diffusion of light by the metal ions to enhance the light absorption.

• 마이크로전자및패키징학회지
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• 제12권3호
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• pp.207-212
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• 2005

Al, Ti, Ta 및 Cr 박막을 DC 마그네트론 스퍼터링방법으로 0 - 800 W의 RF 바이어스로 폴리이미드 기판에 가하면서 증착한 후 금속박막의 접착성을 연구하였다. 접착력은 $90^{\circ}$ 필 테스트로 평가하였다. 필 테스트 결과 모든 시편에서 기판에 RF 바이어스를 가하면 접착력이 향상되었다. RF바이어스를 가한 시편은 필링 도중 계면근처의 폴리이미드 내에서 파괴가 일어나면서 소성변형이 심하게 발생하였다. 단면 투과전자현미경 관찰에 의하면 금속/폴리이미드 계면은 분명하지 않고 복잡한 형상을 띄고 있었다. 이런 복잡한 계면은 RF 바이어스의 영향으로 생겼으며 접착력 향상의 주요 요인이었다.

• 한국마이크로전자및패키징학회:학술대회논문집
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• 한국마이크로전자및패키징학회 2000년도 Proceedings of 5th International Joint Symposium on Microeletronics and Packaging
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• pp.118-118
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• 2000

New single-source precursor, [AlCI3:NH2tBu] was synthesized for AlN thin f film processing with AICI3 (Aluminum Chloride) and tBuNH2 (tert-butylamine). AlN thin films for packaging aspplication were deposited on sapphire substrate by a atmosph하ie-pressure MOCVD. In most of other study methyl-based AI precursors w were used for source, But herein Aluminum Chloride was used for as AI source i in order to prevent the carbon contamination in the films and stabilize the p precursor. New precursor showed the very high gas vapor pressure so it allowed to m make the film under atmospheric-pressure and get the high purified film. High q quality AlN thin film was obtained at 700 to $900^{\circ}C$. The new precursor was p purified by a sublimation technique and help to fabricate high purity film. It s showed high vapor pressure, which is able to a critieal factor for the high purity a and atmospheric CVD of AlN. High Quality AIN thin film was obtained at $700-900^{\circ}C$. The AIN film was characterized by RBS

• 한국재료학회지
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• 제12권3호
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• pp.211-214
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• 2002

Properties of 52/48 PZT films with various thicknesses for piezoelectric micro-electro mechanical systems (MEMS) devices fabricated by multi-coating method on $Pt(3500{\AA})/Ti(400{\AA})/SiO_2(3000{\AA})/Si$(525$\mu\textrm{m}$) substrates were investigated. PZT films were deposited by spin-coating process at 3500 rpm for 30 sec, followed by pyrolysis at 45$0^{\circ}C$ for 10 min producing the thickness of about 120nm. These processes were repeated 4, 8, 12, 16 and 20 times in order to have various thicknesses, respectively. Finally, they were crystallized at $650^{\circ}C$ for 30 min. All thick PZT films showed dense and homogeneous surface microstructures. Thick PZT films showed crystalline structures of random orientations with increasing thickness. Dielectric constants of thick PZT films were increased with increasing film thickness and reached 800 at 100kHz for 2.3$\mu\textrm{m}$ thick PZT film. $P_r\; and\; E_c$ of 2.3$\mu\textrm{m}$ thick PZT films were about 20$\mu$C/$\textrm{cm}^2$ and 63kV/cm. Depth profile analysis by Auger Electron Spectroscopy (AES) of 4800 $\AA$ thick PZT film showed the formation of the perovskite phase on Pt layer by Pb diffusion behavior. It was considered that Pb-Pt intermediate layer promoted PZT (111) columnar structures.

• 한국재료학회지
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• 제21권6호
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• pp.341-346
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• 2011

In this study, we inserted a Zn buffer layer into a AZO/p-type a-si:H layer interface in order to lower the contact resistance of the interface. For the Zn layer, the deposition was conducted at 5 nm, 7 nm and 10 nm using the rf-magnetron sputtering method. The results were compared to that of the AZO film to discuss the possibility of the Zn layer being used as a transparent conductive oxide thin film for application in the silicon heterojunction solar cell. We used the rf-magnetron sputtering method to fabricate Al 2 wt.% of Al-doped ZnO (AZO) film as a transparent conductive oxide (TCO). We analyzed the electro-optical properties of the ZnO as well as the interface properties of the AZO/p-type a-Si:H layer. After inserting a buffer layer into the AZO/p-type a-Si:H layers to enhance the interface properties, we measured the contact resistance of the layers using a CTLM (circular transmission line model) pattern, the depth profile of the layers using AES (auger electron spectroscopy), and the changes in the properties of the AZO thin film through heat treatment. We investigated the effects of the interface properties of the AZO/p-type a-Si:H layer on the characteristics of silicon heterojunction solar cells and the way to improve the interface properties. When depositing AZO thin film on a-Si layer, oxygen atoms are diffused from the AZO thin film towards the a-Si layer. Thus, the characteristics of the solar cells deteriorate due to the created oxide film. While a diffusion of Zn occurs toward the a-Si in the case of AZO used as TCO, the diffusion of In occurs toward a-Si in the case of ITO used as TCO.

• 한국진공학회지
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• 제9권3호
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• pp.221-226
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• 2000

졸겔법 및 진공증착법으로 $WO_3$ 및 $V_2O_5$ 박막을 제조하고, 리튬이온을 이용하여 전기변색 소자를 제작한 후 광학적 특성을 조사하였다. 측정결과 졸겔법으로 제조된 $WO_3$ 박막과 $V_2O_5$ 박막을 수증기 분위기에서 $500^{\circ}C$로 1시간 열처리한 경우 가장 우수한 투과율 변화량을 나타내었다. 정.역방향 동작을 거듭할수록 $WO_3$막의 텅스텐과 ITO막의 인듐이 상호 확산하는 것을 관찰할 수 있었으며 이를 방지하기 위해 수백 $\AA$의 텅스텐 박막을 ITO와 $WO_3$막 사이에 삽입한 결과, cyclic voltamogram의 peak의 감소량이 1/10 이하로 감소하였으며, 리튬이온의 흐름에 의한 인듐과 텅스텐의 이동을 효과적으로 방지할 수 있었다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2009년도 제38회 동계학술대회 초록집
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• pp.131-131
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• 2010

We compared the electrical, optical, structural, and interface properties of indium zinc oxide (IZO)-Ag-IZO and IZO-Au-IZO multilayer electrodes deposited by linear facing target sputtering system at room temperature for organic photovoltaics. The IZO-Ag-IZO and IZO-Au-IZO multilayer electrodes show a significant reduction in their sheet resistance (4.15 and 5.49 Ohm/square) and resistivity ($3.9{\times}10^{-5}$ and $5.5{\times}10^{-5}$Ohm-cm) with increasing thickness of the Ag and Au layers, respectively. In spite of its similar electrical properties, the optical transmittance of the IZO-Ag-IZO electrode is much higher than that of the IZO-Au-IZO electrode, due to the more effective antireflection effect of Ag than Au in the visible region. In addition, the Auger electron spectroscopy depth profile results for the IZO/Ag/IZO and IZO/Au/IZO multilayer electrodes showed no interfacial reaction between the IZO layer and Ag or Au layer, due to the low preparation temperature. To investigate in detail the Ag and Au structures on the bottom IZO electrode with increasing thickness, a synchrotron x-ray scattering examination was employed. Moreover, the OSC fabricated on the IZO-Ag-IZO electrode shows a higher power conversion efficiency (3.05%) than the OSC prepared on the IZO-Au-IZO electrode (2.66%), due to its high optical transmittance in the wavelength range of 400-600 nm, which is the absorption wavelength of the P3HT:PCBM active layer.