• Journal of the Korean Institute of Telematics and Electronics D
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• v.35D no.6
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• pp.79-91
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• 1998

Design principles for high-brightness ligh-temitting diodes have been derived by using escape cone concepts. Based on the design principles, some important high-brightness LED structures developed thus far have been reviewed and, in addition, their external coupling efficiencies have also been estimated. In AlGaAs or InGaAIP LEDs, in which photon absorption in the ohmic electrodes is known to be serious, photon shielding by the electrodes is minimized by using window layer (WL) as well as transparent substrate (TS) leading to significantly improved light-emitting efficiency. However, in InGaN LEDs emitting blue to green lights, the photon absorption in ohmic contact to wide bandgap GaN may be negligible and therefore, photon shielding by the electrodes would not lead to as significant problems as in conventional In AIGaAs or InGaAIP LEDs.

• 전기의세계
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• v.28 no.4
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• pp.53-63
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• 1979

Interface recombination velocity in $Al_{x}$G $a_{1-x}$ As-GaAs and $Al_{0.85}$, G $a_{0.15}$ As-GaA $s_{1-y}$S $b_{y}$ heterojunction systems is studied as a function of lattice mismatch. The results are applied to the design of highly efficient III-V heterojunction solar cells. A horizontal liquid-phase epitaxial growth system was used to prepare p-p-p and p-p-n $Al_{x}$G $a_{1-x}$ As-GaA $s_{1-y}$S $b_{y}$-A $l_{x}$G $a_{1-x}$ As double heterojunction test samples with specified values of x and y. Samples were grown at each composition, with different GaAs and GaAs Sb layer thicknesses. A method was developed to obtain the lattice mismatch and lattice constants in mixed single crystals grown on (100) and (111)B oriented GaAs substrates. In the AlGaAs system, elastic lattice deformation with effective Poisson ratios .mu.$_{eff}$ (100=0.312 and .mu.$_{eff}$ (111B) =0.190 was observed. The lattice constant $a_{0}$ (A $l_{x}$G $a_{1-x}$ As)=5.6532+0.0084x.angs. was obtained at 300K which is in good Agreement with Vegard's law. In the GaAsSb system, although elastic lattice deformation was observed in (111) B-oriented crystals, misfit dislocations reduced the Poisson ratio to zero in (100)-oriented samples. When $a_{0}$ (GaSb)=6.0959 .angs. was assumed at 300K, both (100) and (111)B oriented GaAsSb layers deviated only slightly from Vegard's law. Both (100) and (111)B zero-mismatch $Al_{0.85}$ G $a_{0.15}$As-GaA $s_{1-y}$S $b_{y}$ layers were grown from melts with a weight ratio of $W_{sb}$ / $W_{Ga}$ =0.13 and a growth temperature of 840 to 820 .deg.C. The corresponding Sb compositions were y=0.015 and 0.024 on (100) and (111)B orientations, respectively. This occurs because of a fortuitous in the Sb distribution coefficient with orientation. Interface recombination velocity was estimated from the dependence of the effective minority carrier lifetime on double-heterojunction spacing, using either optical phase-shift or electroluminescence timedecay techniques. The recombination velocity at a (100) interface was reduced from (2 to 3)*10$^{4}$ for y=0 to (6 to 7)*10$^{3}$ cm/sec for lattice-matched $Al_{0.85}$G $a_{0.15}$As-GaA $s_{0.985}$S $b_{0.015}$ Although this reduction is slightly less than that expected from the exponential relationship between interface recombination velocity and lattice mismatch as found in the AlGaAs-GaAs system, solar cells constructed from such a combination of materials should have an excellent spectral response to photons with energies over the full range from 1.4 to 2.6 eV. Similar measurements on a (111) B oriented lattice-matched heterojunction produced some-what larger interface recombination velocities.ities.ities.s.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.48 no.2
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• pp.14-19
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• 2011

We have fabricated GaN Schottky barrier diode (SBD) for high-voltage applications on Si substrate. The leakage current and the electrical characteristics of GaN SBD are investigated by annealing metal-semiconductor junctions. Ohmic junctions of Ti/Al/Mo/Au and Schottky junctions of Ni/Au are used in the fabrication. A test structure is proposed to measured buffer leakage current through a mesa structure. When annealing temperature is increased from $700^{\circ}C$ to $800^{\circ}C$, measured buffer leakage current is also increased from 87 nA to 780 nA at the width of 100 ${\mu}m$. The diffusion of Au, Ti, Mo, O into GaN buffer layer increases the leakage current and that is verified by Auger electron spectroscopy. Experimental results show that the low leakage current and the high breakdown voltage of GaN SBD are achieved by annealing metal-semiconductor junctions.

• Korean Journal of Materials Research
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• v.16 no.8
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• pp.479-484
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• 2006

Highly c-axis oriented poly-crystalline GaN with a dimension of $1{\sim}3\;{\mu}m$ was deposited on $c-Al_2O_3$ substrate by vapor transport epitaxy (VTE) method at the temperature range of $900{\sim}1150^{\circ}C$. XRD intensities from (00'2) plane of grown GaNs were increased with reaction conditions which indicate the improvement of the crystal quality. In the PL spectra measured at 10 K, the spectrum composed with the neutral-donor bound exciton-related emission at 3.47 eV, crystal defect-related emission band at 3.42 eV and with its phonon replicas. The fact that intensity of $I_2$ were increased and FWHM were decreased with growth conditions means that the quality of GaN crystals were improved. With this simple VTE technology, we confirm that the GaNs were simply deposited on sapphire substrate and crystal quality related to optical properties of GaN grown by VTE were relatively good. PL emission without deep level emission in spite of polycrystalline structure can be applicable to the fabrication of large area and low cost optical devices using poly-GaN grown by VTE.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.34 no.1
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• pp.36-39
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• 2024

As interest in power semiconductors is growing recently, research on device design and application using light energy gap materials such as SiC and GaN is being actively conducted. Because AlN single crystals have a larger energy gap than the above mentioned materials, research on high-power devices is also in progress, but commercialized wafers have not yet been reported, so research is needed. In this study, we applied the HVPE (Hydride vapor phase epitaxy) method to produce AlN single crystals and attempted to obtain bulk single crystals using our own manufacturing equipment. To this end, we would like to report the results of securing the growth conditions for single crystals. we would like to report on the change in the shape of the grown crystal according to the change in temperature.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.02a
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• pp.317-318
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• 2013

Terahertz (THz) wave는 광학 영역과 방송파 영역 사이에 광대역 주파수 스펙트럼을 차지하고 있다. X선과는 달리 비이온화 광원으로 직진성, 투과성, 낮은 에너지 (meV)를 가지고 있어 비파괴적이고 무해한 장점을 지니고 있다. 본 연구에서는 In0.53Ga0.47As:Be/In0.52Al0.48As의 multi quantum well (MQW)을 Semi-insulting InP:Fe substrate 위에 active layer의 두께와 적층을 변화주어서 성장하였고Au (200 nm)/Ti (30 nm)의 금속전극으로 공정을 하였다. Ti:Sapphire femtosecond pulse laser를 조사하여 THz time-domain spectrometer 시스템을 이용하여 광전도검출법으로 THz 검출 특성을 연구하였다. THz 검출은 짧은 전하수명과 높은 저항을 요구한다. LTInGaAs의 경우 AsGa antisite로 인하여 짧은 전하수명을 얻게 되면 n-type의 높은 전하밀도를 가지게 되어서 저항이 낮아지게 된다. 높은 저항을 만들기 위하여 Be doping을 이용하여 과잉의 전자들을 보상하고 InAlAs layer를 삽입시켜 보다 높은 저항을 얻었다. LT-InGaAs:Be는 LT-GaAs보다 1/70 정도의 amplitude를 보이는데 LT-InGaAs/InAlAs MQW의 경우 LT-GaAs 대비 약 3/4 정도의 큰 amplitude를 얻었다. 또 active layer의 두께가 얇고 적층이 많을수록 신호가 커지는 것을 알 수 있었다. 이는 상대적으로 band gap이 큰 InAlAs층이 더 높은 저항을 만든 것으로 사료된다.

• Journal of the Korean Institute of Telematics and Electronics D
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• v.34D no.5
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• pp.61-66
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• 1997

In this paper we report the fabrication of an InGaAs metal-semiconductor-metal (MSM) photodiode(PD) which an InAlAs barrier enhancement layer that has very low dark current and high speed chracteristics. The detector using Cr/Au schottky metal fingers with 4um spacing on a large active area of 300*300um$^{2}$ offers a low dark current of 38nA at 10V, a low capacitance of 0.8pF, and a high 3-dB bandwidth of 2.4 GHz. To our knowledge, these characteristics are better than any previously published results obtained from large area InGaAs MSM PD's. The RC equivalent model and frequency domain current response model considering transit time were also used to analyze the frequency characteristic of the fabricated device.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2001.11b
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• pp.221-225
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• 2001

In the paper, we report on the DC and Thermal effect of the GaN based HFET. A physics-based a model was applied and found to be useful for predicting the DC performance and Thermal effect of the GaN based HFET by Various substrate. The performance of device on the sapphire substrates is found to be significantly improve compared with that of a device with an sapphire substrate. The peak drain current of the device achieved at HFET on the SiC substrate

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2011.05a
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• pp.180-181
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• 2011

기존의 GaN LED에 사용되어지고 있는 p형 GaN 반도체의 Ni/Au 투명 접촉 전극을 제조할 때 발생하는 오염과 공정을 줄이고 발광효율을 향상시킬 수 있는 투명 접촉 전극을 제작하기 위해 마그네트론 2원 동시 방전법을 사용하여 AZO-NiO 박막을 증착 하였다. Al 원자 함량에 따른 AZO-NiO 박막의 구조적, 전기적, 광학적 특성을 조사하였다.

• Proceedings of the Korean Vacuum Society Conference
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• 2010.08a
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• pp.2-2
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• 2010

텐덤형 태양전지는 다양한 에너지 대역을 동시에 흡수할 수 있도록 제작할 수 있어 단일접합 태양전지에 비해 높은 에너지변환효율을 기대할 수 있다. 본 연구에서는 GaAs를 기반으로 양자점 혹은 양자우물 구조를 이용한 고효율 텐덤형 태양전지를 설계하고, 완충층 및 활성층의 특성을 분석하였다. 분자선 단결정 성장 장비를 이용하여 GaAs 기판 위에 메타모픽 (metamorphic)성장법을 이용하여 convex, linear, concave 형태로 조성을 변화시켜 $In_xAl_1-_xAs$ 경사형 완충층을 성장한 후 그 특성을 비교하였다. 또한, 최적화된 경사형 완충층 위에 1.1 eV와 1.3 eV의 에너지 대역을 각각 흡수할 수 있는 적층 (5, 10, 15 층)된 InAs 양자점 구조 또는 InGaAs 양자우물구조를 삽입하여 p-n 접합을 성장하였다. 그리고 GaAs/AlGaAs층을 이용한 터널접합에서는 GaAs층의 두께 (20, 30, 50 nm)에 따른 터널링 효과를 평가하였다. 그 결과, 경사형 완충층을 통해 조성 변화로 인한 결함을 최소화하여 다양하게 조성 변화가 가능한 고품위의 구조를 선택적으로 성장할 수 있었으며, 적층의 양자점 구조 및 양자우물 구조를 이용해 고효율 텐덤형 태양전지의 구현 가능성을 확인하였다.