• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.24 no.1
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• pp.1-6
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• 2011

Optical gain characteristics of $1.3{\mu}m$ type-II GaAsSb/InGaNAs/GaAs trilayer quantum well structures were studied using multi-band effective mass theory. The results were compared with those of $1.3{\mu}m$ GaAsSb/InGaNAs/GaAs trilayer quantum well structures. In the case of $1.3{\mu}m$ GaAsSb/InGaNAs/GaAs trilayer quantum well structure, the energy difference between the first two subbands in the valence band is smaller than that of $1.3{\mu}m$ GaAsSb/InGaNAs/GaAs trilayer quantum well structure. Also, $1.3{\mu}m$ GaAsSb/InGaNAs/GaAs trilayer quantum well structure shows larger optical gain than $1.3{\mu}m$ GaAsSb/InGaNAs/GaAs trilayer quantum well structure. This means that GaAsSb/InGaNAs/GaAs system is promising as long-wavelength optoelectronic devices for optical communication.

• Proceedings of the IEEK Conference
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• 1998.06a
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• pp.401-404
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• 1998

Recently, InGaP/GaAs HBTs have been much interested as a potential replacement for AlGaAs/GaAs HBTs because of their superior device and material properties. In this paper, DC characteristics of InGaP/GaAs HBTs and the temperature dependance as well as the reliability were investigated comparing with AlGaAs/GaAs HBTs. As a results InGaP/GaAs HBTs produced the superior performance to AlGaAs/GaAs HBTs.

• Journal of the Korean Institute of Navigation
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• v.16 no.2
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• pp.21-27
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• 1992

Shortening the lasing wavelength(particularly below infrared ; the visible region) of laser diodes is very attractive because it can provide a wide range of applications in the fields of optical information, measurement, sensor, the development of medical instrument, and optical communication through plastic fibers. According to the recent researches on the field, InGaAsP/GaAs was suggested as a material for red-light laser. In this study, in order to grow InGaAsP/GaAs epitaxial layer on InGaAsP/GaAs by LPE, we used GaP and InP two phase solution technique for 670nm and 780 nm region, respectively. Through the X-ray diffraction measurement for the epitaxial layer grown from the experiments, we found that the lattice mismatch of $In_{0.46}Ga_{0.54}As_{0.07}P_{0.93}$/GaAs and $In_{0.19}Ga_{0.81}As_{0.62}P_{0.38}$/GaAs was about +0.3% and +0.1%, respectively.

• Journal of the Semiconductor & Display Technology
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• v.4 no.1 s.10
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• pp.43-48
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• 2005

Metaloganic chemical vapor deposition, also known as metalorganic vapor phase epitaxy has become one of the main techniques for growing thin, high purity films for compound semiconductors such as GaAs, InP, and InGaAsP. In this study, the distribution of growth rate and composition of InGaAsP, InGaP, and InGaAs films are studied using computational method. The influences of process parameters such as pressure, temperature and precursors' partial pressure on the growth rate and composition distributions are analyzed. The film growth rate is increased in the upstream part according to the increase of temperature but not in the downstream part. The Ga composition in InGaAsP film shows an asymptotic behavior for temperature variation but As composition varies significantly within the temperature range considered in the present study. The overall film growth rates of InGaP, InGaAs and InGaAsP are decreased with increasing the Ga/In ratios of the source gases. Pressure variation does not seem to be a significant parameter to the film growth. Film growth characteristics of tertiary films such as InGaP and InGaAs show similar trends to the quaternary film, InGaAsP.

• Journal of the Korean Vacuum Society
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• v.2 no.4
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• pp.424-432
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• 1993

AlGaAs/InGaAs/GaAs pseudomorphic structures have been grown by atmosheric pressure-MOCVD . The Al incorporation efficiency is constant but slightly exceeds the Ga incorporation during the growth of AlGaAs layers at $650^{\circ}C$ . Meanwhile , the In incorporation efficiency is constant but slightly less than the Ga incorporation in InGAAs layers. InGaAs/GaAs QWs were grown and their optical properties were characterized . $\delta$-doped Al0.24Ga0.76As/In0.16 Ga0.84As p-HEMT structures were successfully grown by MOCVD and their transport properties were characterized by Hall effect and SdH measurements. SdH Measurements at 3.7K show clear magnetoresistance oscillations and plateaus in the quantum Hall effect confirming the existence of a two-dimensional electron gas(2DEG) and a parallel conduction through the GaAs buffer layer. The fabricated $1.5\mu\textrm{m}$gatelength p-HEMTs having p-type GaAs in the buffer layer show a high transconductance of 200 mS/mm and a good pinch-off characteristics.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.27 no.6
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• pp.282-288
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• 2017

In this paper, GaAs/AlGaAs multi-layer structure was grown by liquid phase epitaxy with graphite sliding boat, which can be used as a device structure of a photocathode image sensor. The multi-layer structure was grown on an n-type GaAs substrate in the sequence as follows: GaAs buffer layer, Zn-doped p-type AlGaAs layer as etching stop layer, Zn-doped p-type GaAs layer, and Zn-doped p-type AlGaAs layer. The Characteristics of GaAs/AlGaAs structures were analyzed by using scanning electron microscope (SEM), secondary ion mass spectrometer (SIMS) and hall measurement. The SEM images shows that the p-AlGaAs/p-GaAs/p-AlGaAs multi-layer structure was grown with a mirror-like surface on a whole ($1.25mm{\times}25mm$) substrate. The Al composition in the AlGaAs layer was approximately 80 %. Also, it was confirmed that the free carrier concentration in the p-GaAs layer can be adjusted to the range of $8{\times}10^{18}/cm^2$ by hall measurement. In the result, it is expected that the p-AlGaAs/p-GaAs/p-AlGaAs multi-layer structure grown by the LPE can be used as a device structure of a photoelectric cathode image sensor.

• Journal of the Korean Institute of Telematics and Electronics D
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• v.35D no.7
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• pp.88-93
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• 1998

For the self-aligned AlGaAs/GaAs HBTs, the surface states at the interface between the extrinsic base surface and the passivation nitride is a major cause of degradation of dc characteristics. In this paper the degradation mechanisms of self-aligned AlGaAs/GaAs HBT were analyzed, and GaAs HBTs, which employed an InGaP ledge emitter structure formed by the nonself-aligned process to cover the surface of the extrinsic base and reduce the surface states, produced high reliability. Accoridng to the acceleration lifetime test, the nonself-aligned InGaP/GaAs HBTs produced very reliable dc characteristics comparing with the self-aligned AlGaAs/GaAs HBTs. The activation energy was 1.97eV and MTTF $4.8{\times}10^{8}$ hrs at $140^{\circ}C$ which satisfied the MIL standard.

• Journal of the Korean Vacuum Society
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• v.12 no.2
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• pp.118-122
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• 2003

Using low pressure metalorganic chemical vapor deposition (MOCVD), we have developed selectively area epitaxy (SAE). Using the developed SAE technology, we have grown AlGaAs/GaAs multi layers and InGaAs/GaAs quantum wire structures on the selectively $SiO_2$ masked GaAs substrates. We have obtained triangular shaped AlGaAs/GaAs and InGaAs/GaAs structures with sharp tips and smooth sidewalls. To rod the optimum conditions, several growth parameters such as growth rate, V/III ratio, growth temperature, and direction of the opening stripes were investigated. The emission peak from quantum wires was observed at 975 nm. With increasing of temperature the emission intensity from side wall quantum wells decreased abruptly. But the intensity from Quantum wires decreased slowly compared to that of side wall quantum wells and it became even stronger from above 50 K.

• Journal of the Korean Institute of Navigation
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• v.15 no.3
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• pp.99-106
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• 1991

In order to grow InGaAsP epitaxial layer on GaAs by LPE, an accurate phase diagram for In-Ga-As-P quarternary compounds is required. But the short wavelength InGaAsP/GaAs phase diagram for full wavelength range was not yet reported. In this study, therefore, a theoretical calculation has been carried out by using thermodynamic's equation for InGaAsP/GaAs in order to get the relation between the mole fraction of the sloute and solid phase compounds. And the calculation being compared with the dta of Kawanishi et. al, the result has been shown that his phase diagram obtained by the calculation can apply to growing InGaAsP/GaAs by LPE.

• Proceedings of the Korean Vacuum Society Conference
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• 2010.02a
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• pp.89-90
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• 2010

최근 우리는 InGaAs 위에 성장한 InAs 양자점에 GaAs를 얇게 덮음으로써 양자고리를 성장하고, 그 광학적 특성을 분석하였다. [1] 이번 연구에서는 이 양자고리 구조의 전자 구조 및 광학적 특성을 전산모사를 통해 계산하였고, GaAs가 구조의 응력, 압전 포텐셜 및 light-hole 분율에 미치는 영향을 분석하였다. 이론적인 분석을 위해, valence force field 방법을 이용하여 이종 물질간의 격자상수 차이에 의한 격자 변형 및 압전 포텐셜의 변화를 계산하였고, 양자고리 내 전자의 양자화 에너지 및 파동함수를 k p 방법을 통해 얻을 수 있었다. 또한 광학적인 특성 등의 다체 효과를 예측하기 위해 configuration interaction 방법을 사용하였다. 이 연구에서 우리는, GaAs가 InAs에 강한 압축 응력을 가할 것이라는 일반적인 예측과 달리, InGaAs 매트릭스 안에서는 격자상수가 작은 GaAs가 InAs 양자고리에 효과적인 압축 응력을 가할 수 없음을 보였다. 특히 GaAs 층의 두께가 얇을 경우, InGaAs 매트릭스에 의해 인장 응력을 받는 GaAs가 InAs의 응력을 해소하기 충분한 공간을 제공하여, 오히려 InAs의 압축 응력을 약화시키는 것을 알 수 있었다. 이 연구 결과는 응력 분포가 단순한 양자우물 등의 2차원 구조와 달리, 응력 분포가 복잡한 3차원 나노 구조에서는 단순히 격자상수만으로 파장 변화 경향을 예측할 수 없음을 나타낸다. 또한 우리는, GaAs의 큰 negative 이방 응력과 InAs의 작은 positive 이방 응력에 의해 전자와 heavy-hole은 InAs에, light-hole은 GaAs에 구속됨을 보였다. 즉, InAs보다 밴드갭이 큰 GaAs가 전자와 heavy-hole에 대해서는 강한 포텐셜 배리어로 작용하지만 light-hole에 대해서는 포텐셜 우물로 작용하는, 반 우물-반 배리어 특성을 가짐을 알 수 있었다. 이로 인해 GaAs가 있는 양자고리의 light-hole 분율이 GaAs가 없을 경우에 비해 2배에서 8배가량 증가함을 보일 수 있었다. 비슷한 특성이 hole에 대해서는 InP나 InGaAsP 위에 성장한 GaAs 층에서 보고된 바가 있으나, 전자는 InAs로, hole은 GaAs로 분리할 수 있는 3차원 나노 구조에 대한 연구는 이 연구가 처음이다. [2]