• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• 제26권6호
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• pp.441-445
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• 2013

ZnO nanowires on the a-, c- and m-plane oriented 4H-SiC substrates were grown by using a high temperature tube furnace. Ti/Au electrodes were deposited on ZnO nanowires and a-, c- and m-plane 4H-SiC substrates, respectively. The shape and density of the ZnO nanowires were investigated by field emission scanning electron microscope. It was found that the growth direction of nanowires depends strongly on growth parameters such as growth temperature and pressure. In this work, The sensitivity of nanowires formed a-, c- and m-plane oriented 4H-SiC gas sensor was measured at $300^{\circ}C$ with CO gas concentration of 80%. The nanowires grown on a-plane oriented 4H-SiC show improved sensing performance than those on c- and m-plane oriented 4H-SiC due to the increased density of nanowire on a-plane 4H-SiC.

• Journal of the Microelectronics and Packaging Society
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• 제18권3호
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• pp.25-32
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• 2011

We have studied on the slicing and polishing processes of R-plane sapphire wafers for the substrates of UHB nonpolar a-plane GaN LED. The fabrication conditions of the R-plane and c-plane wafers were influenced by the large anisotropic properties (mechanical properties) of the sapphire. The slicing process was more affected by the anisotropic properties of R-plane than the polishing process. When the slicing direction was $45^{\circ}$ to the a-flat, the slicing time was shorter and the quality of as-slicing wafers was better than the slicing direction of normal to the a-flat. The MRR(Material removal rate) of mechanical polishing processes such as lapping and DMP(Diamond mechanical polishing) did not show significant differences between the R-plane and c-plane. The MRR of the c-plane was about two times higher than that of R-planes at the CMP(Chemical mechanical polishing) process due to the formation of hydrolysis reaction layers on the surface of the c-plane.

• Proceedings of the Korean Vacuum Society Conference
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• 한국진공학회 2013년도 제45회 하계 정기학술대회 초록집
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• pp.222-222
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• 2013

GaN 기반 반도체는 넓은 bandgap을 가지고 있어 가시광부터 자외선까지 다양한 광전소자에 유용하게 사용된다. 광전소자중 발광다이오드의 경우 대부분 사파이어 기판위에 성장된다. 하지만 사파이어와 GaN의 격자 불일치 및 열팽창 계수의 차이로 인해 고품질의 GaN를 성장하기가 어렵다. 특히 열팽창 계수의 차이는 GaN 성장 공정이 고온에서 이루어지기 때문에 성장후 상온으로 온도가 떨어질 때 웨이퍼의 bowing을 발생시키고 동시에 dislocation이나 crack과 같은 결함이 생성되 GaN 성장막의 품질을 떨어트린다. 웨이퍼의 크기가 커지면 커질수록 웨이퍼 bowing은 커져 이에 대한 연구는 중요하다. 본 논문에서 2인치 사파이어 기판위에 성장된 GaN의 bow특성을 알아보기 위해 먼저 simulation을 하였고 실제로 성장된 GaN 웨이퍼와 비교를 하였다. c-plane 사파이어 기판위에 성장된 c-plane GaN의 bow특성을 알아보기 위해 성장 온도 $1,100^{\circ}C$에서 GaN두께를 1 ${\mu}m$에서 10 ${\mu}m$까지 1 ${\mu}m$씩 변화시켜 가며 simulation을 하였다. GaN두께가 1 ${\mu}m$일때는 bow가 11 ${\mu}m$, 6 ${\mu}m$ 일때는 54.7 ${\mu}m$, 10 ${\mu}m$ 일때는 108 ${\mu}m$를 얻어 GaN두께가 1 ${\mu}m$씩 증가할 때 마다 bow가 약 10 ${\mu}m$씩 증가하였다. 성장온도에 대한 영향을 알아보기 위해 $700^{\circ}C$에서 $1,200^{\circ}C$까지 $100^{\circ}C$씩 증가시켜며 bow특성 simulation을 하였다. 6 ${\mu}m$성장된 GaN의 경우 성장온도가 $100^{\circ}C$ 씩 증가할 때 bow는 약 6 ${\mu}m$ 증가하였다. 실제 성장된 c-plane GaN웨이퍼와 비교하기 위해 GaN을 각각 3 ${\mu}m$와 6 ${\mu}m$를 성장시켰고 high resolution x-ray diffraction장비를 사용하여 bow를 측정한 결과 각각 28 ${\mu}m$와 61 ${\mu}m$ 였고 simulation결과는 각각 33 ${\mu}m$와 65.5 ${\mu}m$를 얻어 비슷한 결과를 보였다. c-plane 사파이어 기판위에 성장된 c-plane GaN는 방향에 무관하게 동일한 bow 특성을 가지는 반해 r-plane 사파이어 기판위에 성장된 a-plane GaN는 방향에 따라 다른 bow특성을 보인다. a-plane GaN 이방향성적인 bow 특성을 알아보기 위해 simulation을 하였다. $1,100^{\circ}C$에서 a-plane GaN을 성장할 때 두께가 1 ${\mu}m$ 증가할 때마다 bow가 c축 방향으로는 21.7 ${\mu}m$씩 증가하였고 m축 방향으로는 11.8 ${\mu}m$ 씩 증가하여 매우 큰 이방향성적인 bow 특성을 보였다. 실제 r-plane 사파이어 기판위에 성장된 a-plane GaN의 bow를 측정하였고 simulation 결과와 비교해 보았다.

• Journal of the Korean Mathematical Society
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• 제37권3호
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• pp.437-454
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• 2000

Let C be a smooth k-gonal curve of genus g. We study the number of pencils of degree k on C. In case $g\geqk(k-a)/2$ we state a conjecture based on a discussion on plane models for C. From previous work it is known that if C possesses a large number of pencils then C has a special plane model. From this observation the conjectures are split up in two cases : the existence of some types of plane curves should imply the existence of curves C with a given number of pencils; the non-existence of plane curves should imply the non-existence of curves C with some given large number of pencils. The non-existence part only occurs in the range $k(k-1)/2\leqg\leqk(k-1)/2] if k\geq7$. In this range we prove the existence part of the conjecture and we also prove some non-existence statements. Those result imply the conjecture in that range for $k\leq10$. The cases $k\leq6$ are handled separately.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• 제22권5호
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• pp.390-396
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• 2009

The present research was focused to investigate the quality of non-polar SiC substrates grown by a conventional PVT method for optoelectronic applications. The half part of the PVT-grown 6H-SiC crystal boules was sliced along a-direction and m-direction to extensively analyze non-polar planes and then remaining part of that was sliced along the basal plane to produce wafers. The non-polar SiC m-plane and a-plane exhibited apparent peaks around 2 theta=$120^{\circ}$((3-300) plane) and 2 theta=$60^{\circ}$ ((11-20) plane), respectively. FWHM values of m-plane measured along a-direction and c-direction were 60 arc see and 57 arcsec respectively, a-plane measured along m-direction and c-direction were 41 arcsec and 51 arcsec respectively. The typical absorption spectra of SiC crystals indicated that each of SiC crystals were the 6H-SiC with fundamental absorption energy of about 3.04 eV. Non-polar planes contained no micropipe on etched surface. The carrier concentration and mobility of non-polar SiC wafers have estimated by Raman spectrum. It was observed that the carrier mobility is low in the area far from seed crystal with compared to other places.

• Korean Journal of Crystallography
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• 제14권2호
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• pp.93-104
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• 2003

The crystals of group-Ⅲ nitride semiconductors with wurtzite structure exhibit a strong polarity. Especially, GaN has characteristics of different growth rate, anisotropic electrical and optical properties due to the polarity. In this work, GaN epilayer was grown and the polarities of the crystals were observed by the chemical wet etching and SP-EFM. GaN thin films were deposited on c-plane A1₂O₃ substrate under the variations of growth conditions by HVPE such as the deposition temperature of the buffer layer, the deposition time, the ratio of Group-V and Ⅲ and the deposition temperature of the film. The adquate results were obtained under the conditions of 500℃, 90 seconds, 1333 and 1080℃, respectively. It is observed that the GaN layer grown without the buffer layer has N-polarity and the GaN layer grown on the buffer layer has Ga-polarity. Fine crystal single particles were grown on c-plane A1₂O₃ and SiO₂, layer. The external shape of the crystal shows ｛10-11｝｛10-10｝(000-1) planes as expected in the PBC theory and anisotropic behavior along c-axis is obvious. As a result of etching on each plane, (000-1) and ｛10-11｝planes were etched strongly due to the N-polarity and ｛10-10｝ plane was not affected due to the non-polarity. In the case of the crystal grown on c-plane A1₂O₃, two types of crystals were grown. They were hexagonal pyramidal-shape with ｛10-11｝plane and hexagonal prism with basal plane. The latter might be grown by twin plane reentrant edge (TPRE) growth.

• Journal of Ceramic Processing Research
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• 제13권spc2호
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• pp.295-299
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• 2012

We investigated the crystal and the optical properties of GaN-based blue light emitting diodes (LEDs) which were simultaneously grown on c-plane (0001) and semipolar (11-22) GaN templates by using metal-organic chemical vapor deposition (MOCVD). The X-ray rocking curves (XRCs) full width at half maximums (FWHMs) of c-plane (0001) and semipolar (11-22) GaN templates were 275 and 889 arcsec, respectively. In addition, high-resolution X-ray ω-2θ scan showed that satellite peaks of semipolar (11-22) InGaN quantum-wells (QWs) was weaker and broader than that of c-plane (0001) InGaN QWs, indicating that the interface quality of c-plane (0001) QWs was superior to that of semipolar (11-22) QWs. Photoluminescence (PL) and electroluminescence (EL) results showed that the emission intensity and the FWHMs of polar c-plane (0001) LED were much higher and narrower than those of semipolar (11-22) LED, respectively. From these results, we believed that relative poor crystal quality of semipolar (11-22) GaN template might give rise to the poor interfacial quality of QWs, resulting in lower output power than conventional c-plane (0001) GaN-based LEDs.

• Korean Journal of Materials Research
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• 제10권11호
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• pp.784-788
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• 2000

The Vickers microhardness was measured on the basal (0001) plane of sapphire single crystals in the temperature range from 25$^{\circ}C$to 1000$^{\circ}C$. The substructure surrounding the indents was investigated using selective chemical polishing and etching, optical microscopy, and trasmission electron microscopy (TEM). At room temperature, cracks were predominant, and at intermediate temperatures (400$^{\circ}C$and 600$^{\circ}C$), extensive rhombohedral twinning was observed. On the other hand, at higher temperatures, prism plane slip bands on prism plane {1120}(원문참조) were dominant in the microstructure. TEM observations revealed that the dislocation substructure at the vicinity of the indents consisted of fairly straight dislocations lying in basal and/or prism planes and aligned along the <1100> and <1120> directions. The details of the glide dissociation of perfect <110> screw dislocations into three collinear 1/3<1100> partials on the prism plane and the Peierls potential for sapphire single crystals were discussed.

• Journal of the Korean Crystal Growth and Crystal Technology
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• 제25권2호
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• pp.56-61
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• 2015

The effects of the growth temperature on the properties of a-plane GaN epi-layer on r-plane sapphire by HVPE were studied, when the constant V/III ratio and the flow rate of HCl for the Ga source channel was fixed at 10 and 700 sccm, respectively. Additionally the effects of V/III ratios for source gasses were studied when growth temperature and the flow rate of HCl for the Ga source channel was fixed at $1000^{\circ}C$ and 700 sccm, respectively. As the growth temperature was increased, the values of Full Width Half Maximum (FWHM) for Rocking curve (RC) of a-plane GaN (11-20) epi-layer were decreased and thickness of a-plane GaN epi-layer were increased. As V/III ratios were increased at $1000^{\circ}C$, the values of FWHM for RC of a-plane GaN (11-20) were declined and thickness of a-plane GaN epi-layer were increased. The a-plane GaN (11-20) epi-layer grown at $1000^{\circ}C$ and V/III ratio = 10 showed the lowest value FWHM for RC of a-plane GaN (11-20) for 734 arcsec and the smallest dependence of Azimuth angle for FWHM of (11-20) RCs.

• Journal of the Korean Crystal Growth and Crystal Technology
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• 제17권1호
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• pp.6-10
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• 2007

The a-plane GaN layer on r-plane $Al_2O_3$ substrate is grown by mixed-source hydride vapor phase epitaxy (HVPE). The GaN/InGaN heterostructure is performed by selective area growth (SAG) method. The heterostructure consists of a flown over mixed-sourec are used as gallium (or indium) and nitrogen sources. The gas flow rates of HCl and $NH_3$ are maintained at 10 sccm and 500 sccm, respectively. The temperatures of GaN source zone is $650^{\circ}C$. In case of InGaN, the temperature of source zone is $900^{\circ}C$. The grown temperatures of GaN and InGaN layer are $820^{\circ}C\;and\;850^{\circ}C$, respectively. The EL (electroluminescence) peak of GaN/InGaN heterostructure is at nearly 460 nm and the FWHM (full width at half maximum) is 0.67 eV. These results are demonstrated that the heterostructure of III-nitrides on r-plane sapphire can be successfully grown by mixed-source HVPE with multi-sliding boat system.