• Journal of the Korean Institute of Telematics and Electronics
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• v.25 no.10
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• pp.1202-1208
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• 1988

The electron density and electronic states in n- AlGaAs/GaAs heterointerface are calculated by using classical- and quantum-mechanics, respectively. We examine the effects of spacer layer thickness and doping concentration in AlGaAs layer on 2DEG density. Also, the dependences of electronic states of 2DEG upon temperature and acceptor concentration in GaAs layer are investigated.

• Proceedings of the Optical Society of Korea Conference
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• 1995.06a
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• pp.127-137
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• 1995

Anomalously large real space charge transfer through thick barries in GaAs asymmetric double quantum wells is studied by photoluminesence exitation. This inter-well excitonic transfer is very large when the barrier is the Al0.3Ga0.7As alloy, but disappears when the barrier is GaAs/AlAs digital alloy with an equivalent Al concentration of 0.28. These resilts combined with observed x and barrier thickness depence suggest that the spatial fluctuation of the atomic arrangment of Ga and Al in the alloy may be responsible for this transfer. This picture is supported by the quantum mechanical calculation in three dimensions which takes into account the side fluctuation effects.

• Journal of the Korean Institute of Telematics and Electronics D
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• v.36D no.3
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• pp.66-74
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• 1999

InAlGaAs/InGaAs HBTs with the various emitter junction gradings(xf=0.0-1.0) and the modified collector structures (collector- I;n-p-n, collector-II;i-p-n) are simulated and analyzed by HMC (Hybrid Monte Carlo) method in order to find an optimum structure for the shortest transit time. A minimum base transit time($ au$b) of 0.21ps was obtainsed for HBT with the grading layer, which is parabolically graded from $x_f$=1.0 and xf=0.5 at the emitter-base interface. The minimum collector transit time($\tau$c) of 0.31ps was found when the collector was modified by inserting p-p-n layers, because p layer makes it possible to relax the electric field in the i-type collector layer, confining the electrons in the $\Gamma$-valley during transporting across the collector. Thus InAlGaAs/InGaAs HBT in combination with the emitter grading($x_f$=0.5) and the modified collector-III showed the transit times of 0.87 psec and the cut-off frequency (f$\tau$) of 183 GHz.

• Journal of the Korean Wood Science and Technology
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• v.20 no.1
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• pp.23-27
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• 1992

81.9% of the cellulose delignified by acetosolv process was hydrolyzed in HCl-$AlCl_3$ hydrolysis system when $AlCl_3$ was used as catalyst in breaking down of glycosidic bond of cellulose. It was well compared that the HCl hydrolysis system without $AlCl_3$ as catalyst showed only 60~61% of the hydrolyzed yield. Also monosaccharide yield including glucose clearly increased when $AlCl_3$ was use. When concentration of HCl and $AlCl_3$ was increased, the hydrolyzed monosaccharide was increased within certain range. The monosaccharid yield out of the hydrolyzed reached 55.4% at optimum conditions which were identified as 20% of Hel solution, 0.03 Mol of $AlCl_3$, $120^{\circ}C$ of reaction temperature and 7 hours of reaction time employed in this study.

• Journal of the Korean Electrochemical Society
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• v.21 no.1
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• pp.12-20
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• 2018

To solve low cycle efficiency of the zinc anode in Zn-air batteries by corrosion, this study examined the effects of Al as a cathodic protection additive to Zn. The Al-mixed Zn anodes were produced by mixing Zn and Al powder (1, 2, and 3 wt. %). To compare the effects of the Al additive, Si was selected under the same conditions. The morphology and elemental composition of the additives in the Zn were characterized by scanning electron microscopy, energy dispersive X-ray spectroscopy, and inductively coupled plasma - mass spectrometry. The anti-corrosion effects of the Al and Si-mixed Zn anodes were examined by linear polarization. Cyclic voltammetry and charge-discharge tests were conducted to evaluate the electrochemical performance of the Al and Si-mixed Zn anodes. As a result, the Al-mixed Zn anodes showed highest corrosion resistance and cycling performance. Among these, the 2 wt.% Al-mixed Zn anodes exhibited best electrochemical performance.

• Proceedings of the KIEE Conference
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• 2004.07c
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• pp.2020-2021
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• 2004

Distributed optical feedback by gain coupling in V-groove quantum-wire lasers is investigated using InGaAs/AlGaAs active materials grown by metalorganic chemical vapor deposition (MOCVD). In order to avoid grating overgrowth during the fabrication of DFB structures, a newly developed constant MOCVD growth method is employed. Gain anisotropy in emission spectra near Bragg wavelength, resulting from optical feedback along the DFB direction, is clearly observed at room temperature.

• Journal of the Korean Institute of Telematics and Electronics
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• v.27 no.3
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• pp.79-85
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• 1990

Monte Carlo simulation of hot-electron transport in $Al_{0.48}In_{0.52}As/Ga_{0.47}In_{0.53}$ As modulation-doped structure has been performed in which the nonparabolicity in $\Gamma$ valley is taken into account. The calculated results show that the inclusion of the nonparabolicty effect results in a huge decrease in drift velocity.

• Journal of the Korean Ceramic Society
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• v.34 no.5
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• pp.483-490
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• 1997

Al2O3/metal composites were fabricated by oxidation and reaction of molten Al-alloy into two types of commercial Al2O3-SiO2 fibrous insulation board. The growth rate, composition and microstructure of these materials were described. An AlZnMg(7075) alloy was selected as a parent alloy. Mixed polycrystalline fiber and glass phase fiber were used as a filler. The growth surface of an alloy was covered with and without SiO2. SiO2 powder was employed as a surface dopant to aid initial oxidation of Al-alloy. Al-alloy, SiO2, fiber block and growth inhibitor CaSiO3 were packed sequentially in a alumina crucible and oxidized in air at temperature range 90$0^{\circ}C$ to 120$0^{\circ}C$. The growth rate of composite layer was calculated by measuring the mass increasement(g) per unit surface($\textrm{cm}^2$). XRD and optical microscope were used to investigate the composition and phase of composites. The composite grown at 120$0^{\circ}C$ and with SiO2 dopant showed rapid growth rate. The growth behavior differed a little depending on the types of fiber used. The composites consist of $\alpha$-Al2O3, Al, Si and pore. The composite grown at 100$0^{\circ}C$ exhibited better microstructure compared to that grown at 120$0^{\circ}C$.

• Journal of the Korean Ceramic Society
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• v.51 no.3
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• pp.197-200
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• 2014

We investigated the influence of blistering on $Al_2O_3$/SiON stacks and $Al_2O_3$/SiNx:H stacks passivation layers. $Al_2O_3$ film provides outstanding Si surface passivation quality. $Al_2O_3$ film as the rear passivation layer of a p-type Si solar cell is usually stacked with a capping layer, such as $SiO_2$, SiNx, and SiON films. These capping layers protect the thin $Al_2O_3$ layer from an Al electrode during the annealing process. We compared $Al_2O_3$/SiON stacks and $Al_2O_3$/SiNx:H stacks through surface morphology and minority carrier lifetime after annealing processes at $450^{\circ}C$ and $850^{\circ}C$. As a result, the $Al_2O_3$/SiON stacks were observed to produce less blister phenomenon than $Al_2O_3$/SiNx:H stacks. This can be explained by the differences in the H species content. In the process of depositing SiNx film, the rich H species in $NH_3$ source are diffused to the $Al_2O_3$ film. On the other hand, less hydrogen diffusion occurs in SiON film as it contains less H species than SiNx film. This blister phenomenon leads to an increase insurface defect density. Consequently, the $Al_2O_3$/SiON stacks had a higher minority carrier lifetime than the $Al_2O_3$/SiNx:H stacks.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2005.07a
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• pp.46-47
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• 2005

이번 연구는 $BCl_3/CF_4$ 플라즈마를 사용하여 반도체소자 제조 시 널리 이용되는 GaAs 계열반도체 중 대표적인 재료인 GaAs/AlGaAs 및 GaAs/InGaP 구조를 선택적으로 건식 식각한 후 분석한 것이다. 공정변수로는 ICP 소스파워를 0-500W, RIE 파워를 0-50W 그리고 $BCl_3/CF_4$ 가스 혼합비를 중점적으로 변화시켰다. $BCl_3$ 플라즈마만을 사용한 경우 (20$BCl_3$, 20W RIE power, 300W ICP source power, 7.5mTorr) 는 GaAs:AlGaAs의 선택비가 0.5:1 이었으며 이때 GaAs의 식각률은 ~2200${\AA}/min$ 이었으며 AlGaAs의 식각률은 ~4500${\AA}/min$ 이었다. 식각 후 표면의 RMS roughness은 < 2nm로 깨끗한 결과를 보여주었다. 15% $CF_4$ 가스가 혼합된 $17BCl_3/3CF_4$, 20W RIE power, 300W ICP source power, 7.5mTorr의 조건에서 3분 동안 공정한 결과 순수한 $BCl_3$ 플라즈마만을 사용한 경우보다 표면은 다소 거칠었지만 (RMS roughness: ~8.4) GaAs의 식각률 (~980nm/min)과 AlGaAs와 InGaP에 대한 GaAs의 선택도 (GaAs:AlGaAs=16:1, GaAs:InGaP=38:1)는 크게 증가하였다. 그리고 AlGaAs 및 InGaP의 경우 식각 시 나타난 휘발성이 낮은 식각 부산물 ($AlF_3:1300^{\circ}C$, $InF_3:1200^{\circ}C$)로 인하여 50nm/min 이하의 낮은 식각률을 보였고, 62.5%의 $CF_4$가 혼합된 $7.5BCl_3/12.5CF_4$플라즈마의 조건에서는 AlGaAs 및 InGaP에 대한 GaAs의 선택도가 각각 280:1, 250:1을 나타내었다.