• 한국진공학회:학술대회논문집
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• 한국진공학회 1998년도 제14회 학술발표회 논문개요집
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• pp.103-104
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• 1998

GaN is a ppromising materials fot applications in the blue/ultraviolet (UV) light emitting diodes (LEDs)[1] and laser diodes (LDs) [2] High quality ohmic contacts are very critical to these applications since the qualities of ohmic contact system pplay an impportant roles in the high efficient device opperations. For the n-GaN there have been many repports about ohmic contacts and the sppecific contact resistance were as low as from 10-8$\Omega$cm2 However for the ohmic contacts on pp-GaN much fewer study were repported and the sppecific contact resistivity was much lower than of n-GaN. In this ppapper we repport a new Ni/ppt/Au metallization scheme and discuss the mechanism of ohmic formation

• 전자공학회논문지A
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• 제30A권10호
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• pp.27-32
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• 1993

Separate-confinement hetero-structure (SCH) broad area Laser Diodes (LD's) were fabricated from $Al_{0.07}$Ga$_{0.93}$/. As single-quantum-well (SQW) grown by metal organic chemical vapor deposition (MOCVD). Under pulsed operation, we obtained maximum output powers of about 0.8watt/facet and 1.83watt/facet from LD's with 60$\mu$m and 160$\mu$m channel width, respectively, without facet coatings. The differential quantum efficiency of the 60$\mu$m wide LD was about 21.7%/facet and its threshold current density was about 1k [A/cm$^{2}$]. The differential quantum efficiency of the 160$\mu$m wide LD was about 25.6%/facet and its threshold current density was about 1k[A/cm$^{2}$]. The minimum threshold current density of 60$\mu$m wide LD's was 620[A/cm$^{2}$] when the cavity length was 603$\mu$m and the minimum threshold current density of 160$\mu$m wide Ld's was 675[A/cm$^{2}$] when the cavity length was 752$\mu$m. The internal quantum efficienty and the internal loss of both LD's were 92.3% and 18.1cm$^{1}$, respectively.

• 한국광학회지
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• 제16권2호
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• pp.159-161
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• 2005

We report the selective area bandgap tuning of multiple quantum well structures by an impurity free vacancy induced quantum well intermixing technique. A 3dB waveguide directional coupler was fabricated in the disordered section of an intermixed quantum well sample as a demonstration of photonic device applications.

• 한국임상수의학회지
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• 제32권4호
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• pp.295-300
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• 2015

본 연구의 목적은 알지네이트 비드에서 배양한 토끼의 관절 연골세포의 증식과 황산화 글리코스아미노글리칸 합성에 대한 808-nm InGaAs 다이오드 레이저의 효과를 확인하는 것이다. 이전의 연구들에서 서로 다른 종류의 세포에서 레이저의 양성 또는 음성 자극 효과가 알려졌다. 알지네이트 비드 내의 토끼 연골세포에 1.0W 세기의 808-nm InGaAs 다이오드 레이저가 $31J/cm^2$ (1 그룹), $62J/cm^2$ (2 그룹)의 에너지 밀도로 상응하는 그룹에 10초, 20초 동안 24, 48, 72, 96시간째에 각각 조사되었다. 대조군은 처리하지 않았다. 1차 레이저 조사 1주, 2주 후에 MTT 분석이 실시되었다. 황산화 글리코스아미노글리칸 합성은 DMMB 분석을 통해 평가되었다. 조직학적 평가를 위한 세포의 분포와 세포 주변의 황산화 글리코스아미노글리칸 침착은 알시안 블루 염색을 통해 평가되었다. MTT 분석을 통해 알지네이트 비드에서 세포 증식에는 양성 자극 효과가 없음을 알 수 있었다. DMMB 분석을 통해서 2 그룹의 2주차 연골세포에서 황산화 글리코스아미노글리칸 생성이 특이적으로 증가했음을 알 수 있었다. 알시안 블루 염색상에서도 2 그룹 연골세포에서 양성 염색상이 특이적으로 많은 비율을 차지함을 알 수 있었다. 본 연구를 통해 1.0 W 세기의 808-nm InGaAs 다이오드 레이저가 연골세포 증식에 영향이 없으나 알지네이트 비드에서 세포 분비 활동을 자극하여 황산화 글리코스아미노글리칸 침착을 증가시킬 수 있음을 확인하였다.

• ETRI Journal
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• 제30권6호
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• pp.833-843
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• 2008

The effect of forward and reverse electrostatic discharge (ESD) on the electro-optical characteristics of oxide vertical-cavity surface-emitting lasers is investigated using a human body model for the purpose of understanding degradation behavior. Forward ESD-induced degradation is complicated, showing three degradation phases depending on ESD voltage, while reverse ESD-induced degradation is relatively simple, exhibiting two phases of degradation divided by a sudden distinctive change in electro-optical characteristics. We demonstrate that the increase in the threshold current is mainly due to the increase in leakage current, nonradiative recombination current, and optical loss. The decrease in the slope efficiency is mainly due to the increase in optical loss.

• Journal of the Optical Society of Korea
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• 제12권1호
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• pp.57-61
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• 2008

We investigated the laser pulse-width dependence of dense plasmas confined within the magnetic length of $In_{0.2}Ga_{0.8}As$/GaAs multiple quantum wells under high magnetic fields up to 31 T. To fully fill the Landau levels of effectively zero-dimensional system, we used intense femtosecond (fs) laser pulses to create carrier densities near $10^{13}/cm^2$. The observed photoluminescence showed a characteristic of superfluorescence, above critical magnetic field when being excited by pulses shorter than coherence buildup time.

• 한국전기전자재료학회논문지
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• 제17권12호
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• pp.1271-1276
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• 2004

Two-dimensionally arrayed nanocolumn lattices were fabricated by using double-exposure laser holographic method. The hexagonal lattice was formed by rotating the sample with 60 degree while the square lattice by 90 degree before the second laser-exposure. The reactive ion etching for a typical time of 30 min using CH$_4$/H$_2$ plasma enhanced the aspect-ratio by more than 1.5 with a slight increase of the bottom width of columns. The etch-damage was observed by photoluminescence (PL) spectroscopy which was removed by the wet chemical etching using HBr/$H_2O$$_2$/$H_2O$ solution, leading into the enhanced PL intensities of the PCs.

• 한국광학회:학술대회논문집
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• 한국광학회 2003년도 하계학술발표회
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• pp.94-95
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• 2003

최근 들어 저가용 광통신 소자를 제조하기 위한 방법으로 TEC를 사용하지 않는 비냉각형(uncooled) 레이저에 관한 연구가 활발히 진행되고 있다. 이를 위해 반도체 레이저를 형성하는 화합물 반도체 재료 적인 측면에서는 기존에 널리 사용되는 InGaAsP계 물질에 비해 AlGaInAs계 물질구조는 큰 conduction band offset ($\Delta$Ec=$\Delta$O.72Eg) 등으로 인해 고온에서 전자의 overflow를 억제하고 균일한 hole injection으로 인해 우수한 고온특성과 높은 이득(gain)을 보이는 장점을 지니고 있다. (중략)

• 한국재료학회:학술대회논문집
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• 한국재료학회 2003년도 추계학술발표강연 및 논문개요집
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• pp.120-120
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• 2003

The metallic oxide nanomaterials including ZnO, Ga$_2$O$_3$, TiO$_2$, and SnO$_2$ have been synthesized by a number of methods including laser ablation, arc discharge, thermal annealing procedure, catalytic growth processes, and vapor transport. We have been interested in preparing the nanomaterials of Ga$_2$O$_3$, which is a wide band gap semiconductor (E$_{g}$ =4.9 eV) and used as insulating oxide layer for all gallium-based semiconductor. Ga$_2$O$_3$ is stable at high temperature and a transparent oxide, which has potential application in optoelectronic devices. The Ga$_2$O$_3$ nanoparticles and nanobelts were produced using GaN single crystals, which were grown by flux method inside SUS$^{TM}$ cell using a Na flux and exhibit plate-like morphologies with 4 ~ 5 mm in size. In these experiments, the conventional electric furnace was used. GaN single crystals were pulverized in form of powder for the growth of Ga$_2$O$_3$ nanomaterials. The structure, morphology and composition of the products were studied mainly by X-ray diffraction (XRD), field emission scanning electron microscopy (FESEM), and high-resolution transmission electron microscopy (HRTEM).).

• Transactions on Electrical and Electronic Materials
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• 제14권3호
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• pp.148-151
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• 2013

The control of Ga doping in ZnO nanowires (NWs) by physical vapor deposition has been implemented and characterized. Various Ga-doped ZnO NWs were grown using the vapor-liquid-solid (VLS) method, with Au catalyst on c-plane sapphire substrate by hot-walled pulsed laser deposition (HW-PLD), one of the physical vapor deposition methods. The structural, optical and electrical properties of Ga-doped ZnO NWs have been systematically analyzed, by changing Ga concentration in ZnO NWs. We observed stacking faults and different crystalline directions caused by increasing Ga concentration in ZnO NWs, using SEM and HR-TEM. A $D^0X$ peak in the PL spectra of Ga doped ZnO NWs that is sharper than that of pure ZnO NWs has been clearly observed, which indicated the substitution of Ga for Zn. The electrical properties of controlled Ga-doped ZnO NWs have been measured, and show that the conductance of ZnO NWs increased up to 3 wt% Ga doping. However, the conductance of 5 wt% Ga doped ZnO NWs decreased, because the mean free path was decreased, according to the increase of carrier concentration. This control of the structural, optical and electrical properties of ZnO NWs by doping, could provide the possibility of the fabrication of various nanowire based electronic devices, such as nano-FETs, nano-inverters, nano-logic circuits and customized nano-sensors.