• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2001.11a
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• pp.193-196
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• 2001

Single phase CuInS$_2$ thin film with the highest diffraction peak (112) at diffraction angle (2$\theta$) of 27.7$^{\circ}$ and the second highest diffraction peak (220) at diffraction angle (2$\theta$) of 46.25$^{\circ}$ was well made with chalcopyrite structure at substrate temperature of 70 $^{\circ}C$, annealing temperature of 25$0^{\circ}C$, annealing time of 60 min. The CuInS$_2$ thin film had the greatest grain size of 1.2 ${\mu}{\textrm}{m}$ and Cu/In composition ratio of 1.03. Lattice constant of a and c of that CuInS$_2$ thin film was 5.60 $\AA$ and 11.12 $\AA$ respectively. Single phase CuInS$_2$ thin films were accepted from Cu/In composition ratio of 0.84 to 1.3. P-type CuInS$_2$ thin films were appeared at over Cu/In composition ratio of 0.99. Under Cu/In composition ratio of 0.96, conduction types of CuInS$_2$ thin films were n-type. Also, fundamental absorption wavelength, the absorption coefficient and optical energy band gap of p-type CuInS$_2$ thin film with Cu/In composition ratio of 1.3 was 837 nm, 3.0x10 $^4$ $cm^{-1}$ / and 1.48 eV respectively. When CuAn composition ratio was 0.84, fundamental absorption wavelength, the absorption coefficient and optical energy band gap of n-type CuInS$_2$ thin film was 821 nm, 6.0x10$^4$ $cm^{-1}$ / and 1.51 eV respectively.

• Proceedings of the KIEE Conference
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• 2006.07c
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• pp.1649-1650
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• 2006

반도체 소자의 선폭이 나노미터 스케일로 진입함에 따라 소자의 물리적 특성을 나노미터 스케일에서 정밀하게 측정하고자 하는 요구가 증대되고 있다. Atomic Force Microscopy (AFM)은 나노미터 이하의 해상도를 가지고 물질 표면의 기하하적, 전기적 특성 등을 측정할 수 있으므로 나노소자 연구에 필수적인 도구가 되었다. 그러나 AFM은 낮은 측정속도와 탐침의 기하학적 형상에 의한 AFM 영상의 왜곡 등과 같은 치명적인 단점도 가지고 있다. AFM의 낮은 측정 속도를 개선하기 위해서 진보된 마이크로머시닝기술을 이용하여 캔틸레버의 크기를 줄이거나 캔틸레버 위에 박막 구동기를 집적시키는 등의 노력이 진행되고 있으나, 이 경우 전통적인 식각 공정을 이용하여 캔틸레버 위에 tip을 형성하는 것이 매우 어렵다. 본 연구에서는 이미 제작된 캔틸레버 위에 전자빔 조사법을 이용하여 탄소상 tip을 직접 성장시킴으로써 전통적인 식각 공정에 비해 매우 간단하고 값싸며, 활용도가 높은 공정을 개발하였다. 탄소상 tip 성장에 필요한 탄소 소스는 dipping 방법을 이용하여 공급하였고, 시분할법을 사용하여 캔틸레버의 원하는 위치에 tip을 성장시킬 수 있었다. 이렇게 제작된 tip은 최대 $5{\mu}m$ 높이까지 가능했으며, 종횡비는 10:1 이상이어서 tip의 형상에 의한 AFM 영상 왜곡 현상을 최소화할 수 있을 것으로 기대된다.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.31 no.4
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• pp.231-237
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• 2018

In this study, two important requirements for the home production of a robot to detect and remove improvised explosive devices (IEDs) are presented in terms of the total cost for robot system development and the performance improvement of the mine detection technology. Firstly, cost analyses were performed in order to provide a reasonable solution following an engineering estimate method. As a result, the total cost for a mass production system without the mine detection system was estimated to be approximately 396 million won. For the case including the mine detection system, the total cost was estimated to be approximately 411 million won, in which labor costs and overhead charges were slightly increased and the material costs for the mine detection system were negligible. Secondly, a method for fabricating the carbon nanotube (CNT) based gas detection sensor was studied. The detection electrodes were formed by a photolithography process using a photosensitive CNT paste. As a result, this method was shown to be a scalable and expandable technology for producing excellent mine detection sensors. In particular, it was found that surface treatments by using adhesive taping or ion beam bombardment methods are effective for exposing the CNTs to the ambient air environment. Fowler-Nordheim (F-N) plots were obtained from the electron-emission characteristics of the surface treated CNT paste. The F-N plot suggests that sufficient electrons are available for transport between CNT surfaces and chemical molecules, which will make an effective chemiresistive sensor for the advanced IED detection system.

• Applied Microscopy
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• v.37 no.2
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• pp.123-133
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• 2007

The strain fields due to precipitates, especially S-phase $(Al_2CuMg)$ particles in Al-2.5Cu-1.5Mg wt.% alloy were first investigated with Large Angle Convergent Beam Electron Diffraction (LACBED) method. The work involves LACBED pattern simulations to estimate possibly the strength of the strain fields. To do this the morphology of S-particle was optimized as a cylindrical shape with $a_s$ axis, and the displacement vector of strain fields was assumed to be perpendicular to $a_s$ axis. With this simple model the reasonable fittings between the observed patterns of the strain fields and simulations were obtained. And in the early aging stage of the alloy the significant strain fields were not observed. As a result of this study it is expected that the strain fields due to S-phase precipitates in the stage with maximum hardness would make a complex networks to possibly contribute to hardiness of the alloy.

• Journal of the Korea Institute of Military Science and Technology
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• v.15 no.6
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• pp.812-819
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• 2012

Interference and jamming are becoming increasing concern to a radar system nowdays. AESA(Active Electronically Steered Array) antennas and adaptive beamforming(ABF), in which antenna beam patterns can be modified to reject the interference, offer a potential solution to overcome the problems encountered. In this paper, we've developed a planar active phased array radar system, in which ABF, target detection and tracking algorithm operate in real-time. For the high output power and the low noise figure of the antenna, we've designed the S-band TRMs based on GaN HEMT. For real-time processing, we've used wavelenth division multiplexing technique on fiber optic communication which enables rapid data communication between the antenna and the signal processor. Also, we've implemented the HW and SW architecture of Real-time Signal Processor(RSP) for adaptive beamforming that uses SMI(Sample Matrix Inversion) technique based on MVDR(Minimum Variance Distortionless Response). The performance of this radar system has been verified by near-field and far-field tests.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2007.06a
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• pp.151-151
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• 2007

최근에 에피 성장된 ZnO는 UV-LED, 화학적-바이오센서와 투명전도 전극에 많은 관심을 받고 있다. 고 품질의 ZnO는 Metal-organic chemical vapor deposition(MOCVD), Pulsed laser deposition(PLD), molecular beam epitaxy(MBE), 그리고 마그네트론 스퍼터링법에 의해 성장이 이루어지고 있다. 대부분의 ZnO는 사파이어, 싫리콘과 같은 이종 기판 위에 성장되고 있으며, Heteroepitaxy로 성장된 ZnO 박막은 기판과 박막사이의 격자상수, 열팽창계수 차이로 인해 높은 결함 밀도를 보이고 있다. 이러한 문제점은 광전자 소자 응용에 있어 여러 가지 문제점을 야기 시킨다. 이와 같은 문제점을 해결하기 위해 박막과 기판사이에 저온 버퍼층을 사용하거나 같은 물질의 버퍼층을 사용하여 결할 밀도를 감소시키고, 높은 결정성을 가진 ZnO 박막을 성장시킨 결과들이 많이 보고되어지고 있다. 본 연구에서는 마그네트론 스퍼터링 법으로 저온 버퍼층 성장 없이 성장온도 만을 달리 하여 고품질의 ZnO 박막을 성장시켰다. ZnO 박막은 c-sapphire 기판위에 ZnO(99.9999%)의 타겟을 사용하여 $600{\sim}800^{\circ}C$ 온도에서 성장시켰고, 스퍼터링 가스로는 아르곤과 산소를 2:1 비율로 혼합하여 15mtorr의 압력에서 성장하였다. 이렇게 성장시킨 ZnO 박막은 Transmission Electron Microscopy (TEM), High-Resolution X-ray Diffraction (HRXRD), Low-temperature PL, 그리고 Atomic Force Microscopy (AFM)로 특성을 분석 하였다. ZnO 박막은 HRXRD (002) 면의 $\omega$-rocking curve운석 결과, $0.083^{\circ}$의 작은 FEHM을 얻었고, (102) 면의 $\varphi$-sacn을 통해 온도가 증가함에 따라 향상된 6-fold을 확인함으로새 에피성장됨을 알 수 있었다. 또한 TEM분석을 통해 $800^{\circ}C$에서 성장된 박막은 $6.7{\times}10^9/cm^2$의 전위밀도를 얻을 수 있었다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2007.06a
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• pp.11-11
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• 2007

1차원 구조체인 반도체 나노선은 앙자제한효과 (quantum confinement effect) 등을 이용하여 고밀도/고효율의 소자 개발이 기대되고 있다. GaN는 상온에서 3.4 eV의 밴드갭 에너지를 갖는 III-V 족 반도체 재료로써 박막의 경우 광전자 소자로 폭넓게 응용되고 있다. 최근 GaN 나노선의 합성에 성공하면서 발광소자, 고효율의 태양전지, HEMT 등으로의 응용을 위한 많은 연구가 활발히 이루어지고 있다. 하지만, 아직까지 GaN 나노선의 전기적 특성을 제어하는 기술은 확립되지 않고 있다. 본 연구에서는 Vapor solid (VS)법을 이용하여 GaN 나노선을 합성하였으며, GaN 분말과 함께 $Mg_2N_3$ 분말을 첨가하여 (Ga,Mg)N 나노선을 성공적으로 합성하였다. 합성시에 GaN와 Mg 소스간의 거리 변화를 통해 Mg 도핑농도를 제어하고자 하였다. 이 같은 방법으로 합 된 (Ga,Mg)N 나노선의 Mg 도핑농도에 따른 결정학적 특성을 알아보고, (Ga,Mg)N 나노선을 이용하여 소자를 제작한 후 그 전기적 특성을 살펴보고자 한다. X-ray diffraction (XRD)과 high-resolution transmission electron microscopy (HRTEM), EDX를 이용하여 합성된 나노선의 결정학적 특성과 Mg의 도핑 농도를 확인하였다. Photo lithography와 e-beam lithography법을 이용하여 (Ga,Mg)N 나노선 field-effect transistor (FET)를 제작하고, channel current-drain voltage ($I_{ds}-V_{ds}$) 와 channel current-gate voltage ($I_{ds}-V_g$) 측정을 통해 (Ga,Mg)N 나노선이 도핑 농도에 따라 n형에서 p형으로 전기적 특성이 변화함을 확인하였다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2005.07a
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• pp.379-380
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• 2005

Single phase $CuInS_2$ thin film with a highest diffraction peak (112) at a diffraction angle ($2\Theta$) of $27.7^{\circ}$ was well made by SEL method at annealing temperature of $250^{\circ}C$ and annealing hour of 60 min in vacuum of $10^{-3}$ Torr or in S ambience for an hour. And the peak of diffraction intensity at miller index (112) of $CuInS_2$ thin film annealed in S ambience was shown a little higher about 11 % than in only vacuum. Single phase $CuInS_2$ thin films were appeared from 0.85 to 1.26 of Cu/In composition ratio and sulfur composition ratios of $CuInS_2$ thin films fabricated in S ambience were all over 50 atom%. Also when $CuInS_2$ composition ratio was 1.03, $CuInS_2$ thin film with chalcopyrite structure had the highest XRD peak (112). The largest lattice constant of a and grain size of $CuInS_2$ thin film in S ambience was 5.63 ${\AA}$ and 1.2 ${\mu}m$ respectively. And the films in S ambience were all p-conduction type with resistivities of around $10^{-1}{\Omega}cm$.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2006.04a
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• pp.56-57
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• 2006

In this paper, the inorganic multi-layer thin film encapsulation was newly adopted to protect the organic layer from moisture and oxygen. Using the electron beam, Sputter, inorganic multi-layer thin-film encapsulation was deposited onto the Ethylene Terephthalate(PET) and their interface properties between inorganic and organic layer were investigated. In this investigation, the SiON SiO2 and parylene layer showed the most suitable properties. Under these conditions, the WVTR for PET can be reduced from a level of $0.57\;g/m^2/day$ (bare subtrate) to 1*10-5 g/$m^2$/day after application of a SiON and SiO2 layer. These results indicates that the PET/SiO2/SiON/Parylene barrier coatings have high potential for flexible organic light-emitting diode(OLED) applications.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2005.07a
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• pp.207-210
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• 2005

In order to investigate the influence of the homo buffer layer on the microstructure of the ZnO thin film, undoped ZnO buffer layer were deposited on sapphire (0001) substrates by ultra high vaccum pulsed laser deposition (UHV-PLD) and molecular beam eiptaxy (MBE). After high temperature annealing at $600^{\circ}C$ for 30min, undoped ZnO buffer layer was deposited with various oxygen pressure (35~350mtorr). On the grown layer of undoped ZnO, Arsenic-doped(l, 3wt%) ZnO layers were deposited by UHV-PLD. The optical property of the ZnO was analyzed by the photoluminescence (PL) measurement. From $\Theta-2\Theta$ XRD analysis, all the films showed strong (0002) diffraction peak, and this indicates that the grains grew uniformly with the c-axis perpendicular to the substrate surface. Field emission scanning electron microscope (FE-SEM) revealed that microstructures of the ZnO were varied with oxygen pressure, arsenic doping level, and the deposition method of undoped ZnO buffer layers. The films became denser and smoother in the cases of introducing MBE-buffer layer and lower oxygen pressure during As-doped ZnO deposition. Higher As-doping concentration enhanced the columnar-character of the films.