• Journal of Advanced Marine Engineering and Technology
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• v.32 no.3
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• pp.461-467
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• 2008

It was studied the effect of a pre-deposited ultrathin Al layer as part of a buffer layer for the growth of GaN. AlN buffer layers were deposited on a Si(111) substrate using an RF sputtering technique, followed by GaN using hydride vapor phase epitaxy (HVPE). Several atomic layers of Al were deposited prior to AlN sputtering and the samples were compared with the others grown without pre-deposition of Al. And it was also studied the influence of AlN buffer layer thickness on the growth of GaN. The peak wavelength of the photoluminescence (PL) was varied with increasing the thickness of the GaN and AlN layers. The optimum thickness of AlN on a Si(111) substrate with an ultrathin Al layer was about $260{\AA}$. Scanning electron microscope (SEM) images showed coalescent surface morphology and X-ray diffraction (XRD) showed a strongly oriented GaN(0002) peak.

• The Transactions of the Korean Institute of Electrical Engineers
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• v.44 no.2
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• pp.222-227
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• 1995

A new IGBT structure, which may suppress latch-up phenomena considerably, is proposed and verified by MEDICI simulation. The proposed structure employing the segmented $n^{+}$ buffer layer increases latch-up current capability due to suppression of the current flowing through the resistance of $p^{-}$ well, $R_{p}$, which is the main cause of latch-up phenomena without degradation of forward characteristics. The length of the $n^{+}$ buffer layer is investigated by considering the trade-off between the latch-up current capability and the forward voltage drop. The segmented $N^{+}$ buffer layer results in better latch-up immunity in comparison with the uniform buffer layer.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.21 no.6
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• pp.503-508
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• 2008

In order to reduce the piezoelectric field originated from the well layer which resides in InGaN/GaN light emitting diode, InGaN/GaN superlattice buffer layers were grown at the bottom and the top of the active layer. Measuring the photoluminescence spectra with different reverse bias voltages clearly revealed the condition of the flat band under which the transition energy is maximized and the linewidth is minimized. Accordingly, the piezoelectric field of $In_{0.15}Ga_{0.85}N$ in our sample was estimated as -1.08 MV/cm. It is less than half the value reported in the previous studies, and it is evidenced that the strain has reduced due to the superlattice buffer layers.

• KIEE International Transactions on Electrophysics and Applications
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• v.11C no.3
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• pp.43-48
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• 2001

The stability and efficiency of organic light emitting devices are the most critical problems to be solved. The devices based on tris-8-(hydroxyquinoline) aluminum ($Alq_3$) and N,N-diphenyl-N,N-bis(3-methylphenyl)-1, 1-biphenyl-4,4-diamine (TPD) were used to study the effects of buffer layers on their characteristics. We have investigated the characteristic effects of CuPc (copper phthalocyanine) and pentacene buffer layers on the device characteristics, the (5${\sim}$20 nm thick) CuPc layers and the (10${\sim}$20 nm thick) pentacene layers were deposited. Efficiency was slightly improved and the turn-on voltages of the devices with the buffer layers were observed to have lower values than those of the devices without the buffer layers. It is believed that this result is attributed to the improvement of hole injection capability through the buffer layers into hole transport layer (HTL). We have also studied the atomic force microscopic images of the TPD layers deposited on the buffer layer and the bare ITO.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.8 no.3
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• pp.377-382
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• 1998

GaN epilayers having good adhesion and quality were obtained directly on the sapphire {1120} substrates by the OMVPE method without introducing a buffer layer at the lower temperature. The preferred orientations of epilayers turned out to be <0002> and at least 4 kinds of epilayers were competitively grown. Slight distortions of lattices caused by lattice mismatches between sapphire and GaN were observed at the lattices within 2~3 nm region from the interface. Accordingly, TEM investigation revealed that GaN epilayers could be grown on sapphire {1120} planes without a buffer layer.

• Korean Journal of Crystallography
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• v.9 no.2
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• pp.131-137
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• 1998

결정결함의 밀도가 낮은 GaN epitaxy 막을 MOCVD(metal organic chemical vapour deposition) 방법에 의해 성장시켰다. 기판은 6H-SiC를 사용하였으며, AlN과 GaN으로 구성된 이중 buffer 층을 도입하였다. GaN buffer 층은 반응원료인 trimethyl gallium(TMG)과 NH3 가스를 교호식펄스공급(alternating pulsative supply, APS)방법에 의해 만들었다. AlN buffer/6H-SiC 위에 초기단계에 형성되는 GaN 섬은 APS처리에 의해 크기가 커지는 것을 AFM(atomic force microscope)으로 관찰하였다. Buffer 층의 역할은 그 위에 성막시킨 GaN epitaxy 막의 결정성과 결함밀도에 의해 조사하였다. 성막된 GaN의 결정구조와 결정성은 DCXRD(double crystal X-ray diffractormeter)에 의해 측정되었다. 결정결함은 EPD(etching pit density)를 측정하는 방법으로 알칼리혼합용에서 처리된 막을 SEM(scanning electron microscope)으로 관찰하였다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2002.04b
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• pp.53-56
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• 2002

The effect of $\alpha$-septithiophene (${\alpha}-7T$) layers on the organic light emitting diode(OLED) was studied. The ${\alpha}-7T$ was used for a buffer layer in OLED. Hole injection was investigated and improved emission efficiency. The OLEDs structure can be described as indium tin oxide(ITO)/ buffer layer / hole transporting layer / emitting layer / electron transporting layer / LiF / Al. The hole transporting layer were composed of N,N-diphenyl-N,N-di(3-methylphenyl)-1,1-biphenyl-4,4-diamine(TPD), and N,N-di(naphthalene-1-ly)-N,N-diphenyl-benzidine( ${\alpha}$-NPD). The emitting layer, and electron transporting layer consist of tris(8-hydroxyquinolinato) aluminum($Alq_3$). All organic layer were deposited at a background pressure of less than $10^{-6}$ torr using ultra high vacuum (UHV) system. The ${\alpha}-7T$ layer can substitute the hole blocking layer, and improve hole injection properties.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2002.11a
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• pp.534-537
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• 2002

We have studied conduction mechanism that is interpreted in terms of space charge limited current (SCLC) region and tunneling region. The OLEDs are based on the molecular compounds, N,N'-diphenyl-N,N'-bis(3-methylphenyl)-1,1'-biphenyl-4,4'-diamine (TPD) as a hole transport, tris (8- hydroxyquinolinoline) aluminum(III) $(Alq_3)$ as an electron injection and transport and emitting later, copper phthalocyanine (CuPc) and poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) and poly(vinylcarbazole) (PVK) as a buffer layer respectively. Al was used as cathode. We manufactured reference structure that has in ITO/TPD/$Alq_3$/Al. Buffer layer effects were compared to reference structure. And we have analyzed out luminance efficiency-voltage characteristics in ITO/Buffer layer/TPD/$Alq_3$/Al with buffer-layer materials.

• Proceedings of the KIEE Conference
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• 1993.11a
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• pp.240-242
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• 1993

A novel structure, which can suppress latch-up phenomena, is proposed and verified by the PISCESIIB simulation. It is shown that this structure employing the selective N+ buffer layer increases latch-up current density due to suppression of the current flowing through the p-body. The width of the N+ buffer layer is optimized considering the trade-off between the latch-up current density and the forward voltage drop. The selective buffer layer results in an improved trade-off relationship compared with the uniform buffer layer.

• Proceedings of the Korean Vacuum Society Conference
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• 1999.07a
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• pp.119-119
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• 1999

GaN-based 물질들은 blue와 UV 영역의 LED, LD와 같은 광소자가 상용화되었을 뿐만아니라 HBT, FET와 같은 전기소자로도 널리 응용될 시점이지만 아직까지 해결되지 않은 문제점들이 있다. 그 중에 하나가 바로 GaN의 격자상수와 일치하는 기판이 없어 발생하는 dislocation인데, 이를 해결하기 위한 방법으로 새로운 기판이나, buffer, 또는 새로운 성장방법(ELOG) 등을 시도하고 있으나 dislocation density는 아직 높은 (107~1010cm-2) 상태이다. 이에 본 연구에서는 dislocation을 줄이기 위한 방책으로 InxGa1-xN를 새로운 buffer층으로 사용하여 GaN 박막을 MBE 방법으로 성장하였다. InxGa1-xN를 선택한 이유는 GaN와의 격자상수차이가 In0.12Ga0.88N일 경우 거의 일치한다는 보고가 있으며, 특히 InGaN의 melting point는 GaN의 성장온도 보다는 약간 높기 때문에 GaN 박막을 성장할 때와 식힐 때의 InGaN 원자결합은 약하게 작용되며, 결국 이는 열적인 stress를 줄여주게 된다. 이와 같이 성장된 GaN 박막은 그 결정성을 XRD로 분석하였고, 표면과 계면을 SEM으로 관찰하였다. 그리고 그 광학적 특성을 저온 PL로서 조사하였다. 그 결과를 살펴보면 35$^{\circ}$ 근방에서 GaN(0002) peak가 나온 것으로 보아 wurtzite 구조가 성장됨을 XRD로부터 확인하였다. 그리고 저온 (12K) PL에서는 3.470eV의 D$^{\circ}$X peak뿐만 아니라 3.258eV에 해당하는 peak를 얻었는데, 이는 InxGa1-xN buffer layer의 vapour pressure가 높은 (<50$0^{\circ}C$)에 도달하게 됨으로써 dissociation이 일어나면서 초기 성장이 이루어졌고 이는 다시 계면에서의 inter-diffusion을 발생시킨 것으로 보여진다.