• Title/Summary/Keyword: GaAs(100)표면

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Comparison of Dry Etching of AlGaAs/GaAs in High Density Inductively Coupled $BCl_3$ based Plasmas ($BCl_3$에 기초한 고밀도 유도결합 플라즈마에 의한 AlGaAs/GaAs 건식식각 비교)

  • ;;;;;S. J. Pearton
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2003.03a
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    • pp.63-63
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    • 2003
  • 플라즈마 공정은 DRAM, 이종접합 양극성 트랜지스터(HBTs), 레이저, 평면도파로(planar lightwave circuit)와 같은 전자소자 및 광조자 제작에 있어서 핵심 공정중의 하나이다. 최근 미세 구조의 크기가 극도로 감소하게 됨에 따라 실제 소작 제작에 있어서 미세한 모양을 식각하는 공정이 매우 중요하게 되었다. 그 중에서 고밀도 유도결합 플라즈마(high density inductively coupled plasma)를 이용한 기술은 빠르고 정확한 식각률, 우수한 식각 균일도와 높은 재현성 때문에 습식식각 기술보다 선호되고 있다. 본 연구는 평판형(planar) 고밀도 유도결합 플라즈마 식각장치를 이용하여 BCl$_3$와 BCl$_3$/Ar 플라즈마에 따른 AlGaAs/GaAs의 식각결과를 비교 분석하였다. 공정 변수는 ICP 소스(source power)파워, RIE 척(chuck) 파워, 공정 압력, 그리고 Ar 조성비(0-100%)이었다. BCl$_3$에 Ar을 첨가하게 되면 순수한 BCl$_3$ 플라즈마에서의 AlGaAs/GaAs 식각률(> 3000 $\AA$/min) 보다 분당 약 1000$\AA$ 이상 높은 식각률(>4000 $\AA$/min)을 나타내었다. 이 결과는 Ar 플라즈마의 이온보조(ion-assisted)가 식각률 증가에 기인한다고 예측된다. 그리고 전자주사 현미경(SEM)과 원자력간 현미경(AFM)을 사용하여 식각 후 표면 거칠기 및 수직 측벽도 둥을 분석하였다. 마지막으로 XPS를 이용하여 식각된 후에 표면에 남아 있는 잔류 성분 분석을 연구하였다. 본 결과를 종합하면 BCl$_3$에 기초한 평판형 유도결합 플라즈마는 AlGaAs/GaAs 구조의 식각시 많은 우수한 특성을 보여주었다.79$\ell/\textrm{cm}^3$, 0.016$\ell/\textrm{cm}^3$, 혼합재료 2는 0.045$\ell/\textrm{cm}^3$, 0.014$\ell/\textrm{cm}^3$, 혼합재료 3은 0.123$\ell/\textrm{cm}^3$, 0.017$\ell/\textrm{cm}^3$, 혼합재료 4는 0.055$\ell/\textrm{cm}^3$, 0.016$\ell/\textrm{cm}^3$, 혼합재료 5는 0.031$\ell/\textrm{cm}^3$, 0.015$\ell/\textrm{cm}^3$, 혼합재료 6은 0.111$\ell/\textrm{cm}^3$, 0.020$\ell/\textrm{cm}^3$로 나타났다. 3. 단일재료의 악취흡착성능 실험결과 암모니아는 코코넛, 소나무수피, 왕겨에서 흡착능력이 우수하게 나타났으며, 황화수소는 펄라이트, 왕겨, 소나무수피에서 다른 재료에 비하여 상대적으로 우수한 것으로 나타났으며, 혼합충진재는 암모니아의 경우 코코넛과 펄라이트의 비율이 70%:30%인 혼합재료 3번과 소나무수피와 펄라이트의 비율이 70%:30%인 혼합재료 6번에서 다른 혼합재료에 비하여 우수한 것으로 나타났으며, 황화수소의 경우 혼합재료에 따라 약간의 차이를 보였다. 4. 코코넛과 소나무수피의 경우 암모니아가스에 대한 흡착성능은 거의 비슷한 것으로 사료되며, 코코넛의 경우 전량을 수입에 의존하고 있다는 점에서 국내 조달이 용이하며, 구입 비용도 적게 소요되는 소나무수피를 사용하는 것이 경제적이라고 사료된다. 5. 마지막으로 악취제거 미생물균주를 접종한 소나무수피 70%와 펄라이트 30%의 혼합재료를 24시간동안 장기간 운전

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Generation of Longitudinal Twin of GaAs Single Crystal by LEC Method (LEC법 GaAs 단결정의 종단쌍정 발생)

  • Gang, Jin-Gi;Yu, Hak-Do;Park, Jong-Mok
    • Korean Journal of Crystallography
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    • v.2 no.1
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    • pp.1-11
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    • 1991
  • When GaAs single crystals are grown by LEC method, a serious problem is that longitudinal twins are often generated. the growth axis is changed from (100) to (221) direction by logitudinal twin. In this experiment, 3 inch GaAs single crystals, slaving (100) uonh axis, were von by LEC method. Striations and edge facets generated during crystal growth, were observed by SPW photo-etching. Relationship between striations and edge facets was studied. Instability of their generation was the cause of goneration of longitudinal twins. The shape of striations was changed with the growth conditions such as crystal diameter and melt volume. In the region of crystal edge: there was the microscopic fluctuation by the instability of melt convection. Edge facets consisting of {111} plane developed well in the region which striation were convex to the melt. Because the angle between striation and {111} edge facet decreased in that region. Longitudinal twins were generated on the crystal surface at the <111> direction which is perpendicular to the growth axis. These were generated by unstable melt convection and propagated in the crystal as crystal grew. Longitudinal twins were generated when regrowth rate was very fast after {111} edge facets were remelted. So, in order to supress the generation of longitudinal twin, abrupt change of melt convection must be prohibited.

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Influence of the Diamond Abrasive Size during Mechanical Polishing Process on the Surface Morphology of Gallium Nitride Substrate (Gallium Nitride 기판의 Mechanical Polishing시 다이아몬드 입자 크기에 따른 표면 Morphology의 변화)

  • Kim, Kyoung-Jun;Jeong, Jin-Suk;Jang, Hak-Jin;Shin, Hyun-Min;Jeong, Hae-Do
    • Journal of the Korean Society for Precision Engineering
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    • v.25 no.9
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    • pp.32-37
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    • 2008
  • Freestanding hydride vapor phase epitaxy grown GaN(Gallium Nitride) substrates subjected to various polishing methods were characterized for their surface and subsurface conditions, Although CMP(Chemical Mechanical Polishing) is one of the best approaches for reducing scratches and subsurface damages, the removal rate of Ga-polar surface in CMP is insignificant($0.1{\sim}0.3{\mu}m$/hr) as compared with that of N-polar surface, Therefore, conventional MP(Mechanical Polishing) is commonly used in the GaN substrate fabrication process, MP of (0001) surface of GaN has been demonstrated using diamond slurries with different abrasive sizes, Diamond abrasives of size ranging from 30nm to 100nm were dispersed in ethylene glycol solutions and mineral oil solutions, respectively. Significant change in the surface roughness ($R_a$ 0.15nm) and scratch-free surface were obtained by diamond slurry of 30nm in mean abrasive size dispersed in mineral oil solutions. However, MP process introduced subsurface damages confirmed by TEM (Transmission Electronic Microscope) and PL(Photo-Luminescence) analysis.

Structural and Optical Characteristics of InAs/InAlGaAs Quantum Dots Grown on InP/InGaAs/InP Distributed Feedback Grating Structure (InP/InGaAs/InP 분포귀환형 회절격자 위에 성장된 InAs/InAlGaAs 양자점의 구조적.광학적 특성)

  • Kwack, H.S.;Kim, J.S.;Lee, J.H.;Hong, S.U.;Choi, B.S.;Oh, D.K.;Cho, Y.H.
    • Journal of the Korean Vacuum Society
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    • v.15 no.3
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    • pp.294-300
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    • 2006
  • We fabricated the distributed feedback (DFB) InP/InGaAs/InP grating structures on InP (100) substrates by metal-organic chemical vapor deposition, and their structural properties were investigated by atomic force microscopy and scanning electron microscopy. Self-assembled InAs/InAlGaAs quantum dots (QDs) were grown on the InP/InGaAs/InP grating structures by molecular beam epitaxy, and their optical properties were compared with InAs/InAlGaAs QDs without grating structure. The duty of the grating structures was about 30%. The PL peak position of InAs/InAlGaAs QDs grown on the grating structure was 1605 nm, which was red-shifted by 18 nm from that of the InAs/InAlGaAs QDs without grating structure. This indicates that the formation of InAs/InAlGaAs QDs was affected by the existence of the DFB grating structures.

A Study on the Growth of $In_{0.53}Ga_{0.47}As/In_{0.52}AI_{0.48}$As/InP Epitaxial Layers for HEMT by MBE (MBE에 의한 HEMT 소자용 $In_{0.53}Ga_{0.47}As/In_{0.52}AI_{0.48}$As/InP 에피택셜층 성장 연구)

  • 노동완;이해권;이재진;이재진;편광의;남기수
    • Journal of the Korean Vacuum Society
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    • v.4 no.2
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    • pp.177-182
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    • 1995
  • 저잡음 HEMT소자 제작을 위한 에피택셜 기판을 MBE방법을 이용하여 $In_{0.53}Ga_{0.47}As/In_{0.52}AI_{0.48}$As/InP 물질계로 성장하였다. 기판온도의 변화, 채널층과 격리층 사이의 성장 일시 멈춤 등의 성장 조건 변화에 따른 Hall 이동도의 변화를 연구하였다. 전자 공급층을 Si으로 델타도핑한 결과 같은 조건에서 성장기판의 온도를 $520^{\circ}C$에서$ 540^{\circ}C$로 증가시키면 실온의 전자이동도는 7,850$\textrm{cm}^2$/Vsec으로 증가하였으며, 격리층과 채널층 사이에서 약 50초간 성장중 채널층의 표면 adatom의 surface migration 시간을 충분히 제공하여 결정결함의 감소로 계면의 급격성이 향상된 결과로 사료된다. 본 실험을 통하여 얻은 최고 이동도 값은 격리층의 두께가 $100\AA$인 경유에 상온 측정결과 $11,400\textrm{cm}^2$/vsec 및 77K 측정결과 $50,300\textrm{cm}^2$/Vsec이었다.

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Fabrication of Nanopatterned Oxide Layer on GaAs Substrate by using Block Copolymer and Reactive Ion Etching (블록 공중합체와 반응성 이온식각을 이용한 GaAs 기판상의 나노패터닝된 산화막 형성)

  • Kang, Gil-Bum;Kwon, Soon-Mook;Kim, Seoung-Il;Kim, Yong-Tae;Park, Jung-Ho
    • Journal of the Microelectronics and Packaging Society
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    • v.16 no.4
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    • pp.29-32
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    • 2009
  • Dense and periodic arrays of nano-sized holes were patterned in oxide thin film on GaAs substrate. To obtain the nano-size patterns, self-assembling diblock copolymer was used to produce thin film of uniformly distributed parallel cylinders of polymethylmethacrylate (PMMA) in polystyrene (PS) matrix. The PMMA cylinders were removed with UV expose and acetic acid rinse to produce PS nanotemplate. By reactive ion etching, pattern of the PS template was transferred to under laid silicon oxide layer. Transferred patterns were reached to the GaAs substrate by controlling the dry etching time. We confirmed the achievement of etching through the removing oxide layer and observation of GaAs substrate surface. Optimized etching time was 90 to 100 sec. Pore sizes of the nanopattern in the silicon oxide layer were 20~22 nm.

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Depleted optical thyristor - Laser Diode using surface-normal injection method (표면 수직 입사 방식의 완전 공핍 광 싸이리스터 레이저 다이오드)

  • choi, Yoon-Kyung;Kim, Doo-Keun;Choi, Young-Wan;Lee, Suk;Woo, Duck-Hwa;Byun, Young-Tae;Kim, Jae-Hun;Kim, Sun-Ho
    • Proceedings of the Optical Society of Korea Conference
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    • 2004.07a
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    • pp.26-27
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    • 2004
  • We present the first demonstration of the vertical-injection depleted optical thyristor laster diode with InGaAs/InGaAsP multiple quantum well structure. The measured switching voltage and current are 3.36 V and 10 A respectively. The holding voltage and current are respectively 1.37 V, 100 A. The lasing threshold current is 131 mA at 25 C. The output peak wavelength is at 1578 nm at a bias current equal to 1.22 times threshold.

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Characterization of various crystal planes of beta-phase gallium oxide single crystal grown by the EFG method using multi-slit structure (다중 슬릿 구조를 이용한 EFG 법으로 성장시킨 β-Ga2O3 단결정의 다양한 결정면에 따른 특성 분석)

  • Hui-Yeon Jang;Su-Min Choi;Mi-Seon Park;Gwang-Hee Jung;Jin-Ki Kang;Tae-Kyung Lee;Hyoung-Jae Kim;Won-Jae Lee
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.34 no.1
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    • pp.1-7
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    • 2024
  • β-Ga2O3 is a material with a wide band gap of ~4.8 eV and a high breakdown-voltage of 8 MV/cm, and is attracting much attention in the field of power device applications. In addition, compared to representative WBG semiconductor materials such as SiC, GaN and Diamond, it has the advantage of enabling single crystal growth with high growth rate and low manufacturing cost [1-4]. In this study, we succeeded in growing a 10 mm thick β-Ga2O3 single crystal doped with 0.3 mol% SnO2 through the EFG (Edge-defined Film-fed Growth) method using multi-slit structure. The growth direction and growth plane were set to [010]/(010), respectively, and the growth speed was about 12 mm/h. The grown β-Ga2O3 single crystal was cut into various crystal planes (010, 001, 100, ${\bar{2}}01$) and surface processed. The processed samples were compared for characteristics according to crystal plane through analysis such as XRD, UV/VIS/NIR/Spec., Mercury Probe, AFM and Etching. This research is expected to contribute to the development of power semiconductor technology in high-voltage and high-temperature applications, and selecting a substrate with better characteristics will play an important role in improving device performance and reliability.

Effect of thickness of GaAs buffer layer on the structural properties of CdTe films (GaAs 완충층을 사용한 CdTe박막의 성장 특성)

  • Kim, Kwang-Chon;Jung, Kyoo-Ho;You, Hyun-Woo;Yim, Ju-Hyuk;Kim, Hyun-Jae;Kim, Jin-Sang
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.06a
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    • pp.247-247
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    • 2010
  • CdTe는 최근 적외선 검출기 개발에 응용하기 위해 활발한 연구가 진행 중인데 이는 HgCdTe(MCT)와 격자 불일치가 0.3% 이하로 대구경 단결정 MCT박막 제작이 용이하기 때문이다. 본 연구에서는 MBE 공정으로 GaAs 물질이 완충층으로 증착된 Si(100)기판을 사용하여 CdTe 물질과 Si기판간의 격자 불일치를 줄여 대면적 CdTe 단결정 박막을 얻고자 완충층의 두께별 결정성 및 표면 특성을 보았다. CdTe 박막의 증착은 Metal Organic Chemical Vapor Deposition system (MOCVD)를 이용하였고 실험결과 2nm의 GaAs 완충층이 사용된 박막에서 단결정 CdTe(400) 박막이 성장 되었으며, GaAs 완충층의 두께가 증가 함에 따라 $1{\mu}m$ 완충층에서는 다결정 박막이 성장 되었다. 본 연구결과는 Si 기판에 성장된 단결정 CdTe층을 이용 대면적 HgCdTe웨이퍼의 제조에 널리 이용 될 수 있으리라 여겨진다.

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Properties of Ga-doped ZnO transparent conducting oxide fabricated on PET substrate by RF magnetron sputtering (RF 마그네트론 스퍼터링 공정으로 PET 기판 위에 제조한 Ga-doped ZnO 투명전도막의 특성)

  • Kim, Jeong-Yeon;Kim, Byeong-Guk;Lee, Yong-Koo;Kim, Jae-Hwa;Woo, Duck-Hyun;Kweon, Soon-Yong;Lim, Dong-Gun;Park, Jae-Hwan
    • Journal of the Microelectronics and Packaging Society
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    • v.17 no.1
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    • pp.19-24
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    • 2010
  • The effects of $O_2$ plasma pretreatment on the properties of Ga-doped ZnO films on PET substrate were studied. GZO films were fabricated by RF magnetron sputtering process. To improve surface energy and adhesion between the PET substrate and the GZO film, $O_2$ plasma pretreatment process was used prior to GZO sputtering. As the RF power and the treatment time increased, the crystallinity increased and the contact angle decreased significantly. When the RF power was 100 W and the treatment time was 600 sec in $O_2$ plasma pretreatment process, the resistivity of GZO films on the PET substrate was $1.90{\times}10^{-3}{\Omega}-cm$.