• Title/Summary/Keyword: epitaxy

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Photoluminescence Characteristics of ZnO Nano Needle-like Rods grown by the Hot Wall Epitaxy Method

  • Eom, Sung-Hwan;Choi, Yong-Dae
    • Transactions on Electrical and Electronic Materials
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    • v.8 no.5
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    • pp.191-195
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    • 2007
  • We investigated photoluminescence characteristics of ZnO nano needle-like rods grown on a c-plane $AL_2O_3$ substrate by the hot wall epitaxy method. The nano-rods were vertically well aligned along the ZnO c-axis. The diameters of the ZnO nano-rods ranged from 20 nm to 30 nm and their lengths were between 600 and 700 nm. In the photoluminescence spectrum at 10 K, the exciton emission bound to the neutral donor dominated while defect related emission was weakly observed. With a further increase of temperature, the free exciton emission appeared and eventually became dominant at room temperature.

Magnetic Properties of La-doped YIG Films Prepared by LPE(Liquid Phase Epitaxy) (LPE 성장법으로 성장시킨 La을 첨가한 YIG 막의 자성특성)

  • 김동영;한진우;김명수;이상석
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.14 no.3
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    • pp.257-262
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    • 2001
  • Single crystalline films of La doped YIG(yttrium iron garnet) were grown by the liquid phase epitaxy. The lattice constants of films obtained by DCD(double crystalline diffractometer) measurement increased with increasing La contents in films. In particular, lattice constants of films grown wiht Y/La=20 solution were nearly same as those of GGG (gadolinium gallium garnet) substrate. The saturation magnetization measured with VSM (vibrating sample magnetometer) was about 1750Gauss which is the same as that of pure YIG irrespective of La contents in films. FMR(ferromagnetic resonance) linewidth of La doped YIG was smaller than that of pure YIG. Since appropriate La doping decreases the lattice mismatch between film and substrate, the FMR linewidth was Y/La=20 in this experiment.

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Selective Area Epitaxy of GaAs and InGaAs by Ultrahigh Vacuum Chemical vapor Deposition(UHVCVD) (Ultrahigh Vacuum Chemical Vapor Deposition (UHVCVD)법에 의한 GaAs와 InGaAs 박막의 선택 에피택시)

  • 김성복
    • Journal of the Korean Vacuum Society
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    • v.4 no.3
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    • pp.275-282
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    • 1995
  • III족 원료 가스로 triethylgallium(TEGa)과 trimethylindium(TMIn)을 사용하고 V족 원료 가스로 사전 열 분해하지 않은 arsine(AsH3)과 monoethylarsine(MEAs)을 사용하여 ultrahigh vacuum chemical vapor deposition(UHVCVD)법으로 Si3N4로 패턴된 GaAs(100)기판 위에 GaAs와 InGaAsqkr막을 선택적으로 에피택시 성장을 하였다. V족 원료 가스를 사전 열 분해하지 않으므로 넓은 성장 온도 구간과 V/lll 비율에서도 선택적으로 박막이 성장되었다. 또한 선택 에피택시의 성장 메카니즘을 규명하기 위하여 다양한 filling factor(전체면적중 opening된 면적의 비율)를 가지는 기판을 제작하여 성장에 사용하였다. UHVCVD법에서는 마스크에 면적중 opening된 면적의 비율)를 가지는 기판을 제작하여 성장에 사용하였다. UHVCVD법에서는 마스크에 입사된 분자 상태의 원료 기체가 탈착된 후 표면 이동이나 가스 상태의 확산과정 없이 마스크로부터 제거되므로 패턴의 크기와 모양에 따른 성장 속도의 변화나 조성의 변화가 없을 뿐만 아니라 chemical beam epitaxy(CBE)/metalorganic molecular beam epitaxy(MOMBE)법에서 알려진 한계 성장온도 이하에서 선택 에피택시 성장이 이루어졌다.

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Growth of GaN on ZnO Substrate by Hydride Vapor-Phase Epitaxy (ZnO 기판 위에 Hydride Vapor-Phase Epitaxy법에 의한 GaN의 성장)

  • Jo, Seong-Ryong;Kim, Seon-Tae
    • Korean Journal of Materials Research
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    • v.12 no.4
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    • pp.304-307
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    • 2002
  • A zinc oxide (ZnO) single crystal was used as a substrate in the hydride vapor-phase epitaxy (HVPE) growth of GaN and the structural and optical properties of GaN layer were characterized by x- ray diffraction, transmission electron microscopy, secondary ion mass spectrometry, and photoluminescence (PL) analysis. Despite a good lattice match and an identical structure, ZnO is not an appropriate substrate for application of HVPE growth of GaN. Thick film could not be grown. The substrate reacted with process gases and Ga, being unstable at high temperatures. The crystallinity of ZnO substrate deteriorated seriously with growth time, and a thin alloy layer formed at the growth interface due to the reaction between ZnO and GaN. The PL from a GaN layer demonstrated the impurity contamination during growth possibly due to the out-diffusion from the substrate.

Photoreflectance of A $I_x$Ga${1-x}$As(x.<=.0.15) grown by liquid-phase epitaxy (Liquid-phase epitaxy로 성장시킨 A $I_x$Ga${1-x}$As(x.<=.0.15)의 photoreflectance)

  • 배인호;김인수;이철욱;최현태;김말문;김상기
    • Electrical & Electronic Materials
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    • v.7 no.4
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    • pp.300-305
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    • 1994
  • We determined the alloy composition of the liquid-phase epitaxy(LPE) grown $Al_{x}$G $a_{1-x}$ As by the photoreflectance(PR), and observed the variation of PR signal by changing the condition of annealing and thickness of epilayer. As the measuring temperature was decreased, the broadening parameter was decreased, and the amplitude of PR signal was increased. When the temperature of annealing was increased, the surface carrier concentration was decreased and then the shape and amplitude of PR signal were affected by the surface electric field. The structure change was observed when the specimen was annealed for long time at a high temperature. We found that the surface electric field increased when the thickness of epilayer was decreased by etching, because the band bending was increased by the decreased of the width of depletion layer....

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Magnetic Properties of La-doped YIG films prepared by LPE(Liquid Phase Epitaxy) (LPE 성장법으로 성장시킨 La 을 첨가한 YIG 막의 자성특성)

  • 김동영;한진우;김명수;이상석
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.11a
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    • pp.89-92
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    • 2000
  • Liquid Phase Epitaxy 법을 이용하여 La이 첨가된 YIG(Yitrium Ion Garnet)막을 성장시켰다. X선 회절 분석을 이용하여 La의 첨가량을 변화시키며 제조된 막의 격자상수를 조사한 결과, La의 첨가량이 증가함에 따라 성장된 막의 격자상수도 증가하였으며 Y/La이 20인 경우, 막의 격자상수가 기판으로 사용한 GGG의 격자상수와 일치하였다. VSM(Vibration Sample Magnetometer)를 이용하여 구한 막의 포화자화 값은 La의 첨가량과 관계없이 순수한 YIG의 경우와 같은 값인 1750정도로 거의 일정하였다. FMR(Ferro Magnetic Resonance) 측정장치를 이용한 막의 강자성 공명선폭을 측정결과 막의 공명선폭은 La의 첨가량과 관계없이 모든 경우에 순수한 YIG보다 감소하였다. 실험범위내의 La의 첨가에 대해서 기판과의 격자불일치가 순수한 YIG의 경우보다 감소하기 때문이다. La의 첨가량이 많은 조건에서 성장시킨 막은 공명선폭이 크고 두께의 증가에 따라서 선폭이 증가하였으며, Y/La가 20과 30일 때 성장시킨 막에서는 공명선폭의 절대값도 작고 두께에 따른 공명선폭의 변화도 관찰되지 않았다.

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Metal-Organic Vapor Phase Epitaxy III. Atomic Layer Epitaxy (MOVPE 단결정층 성장법 III. 원자층 성장법)

  • 정원국
    • Journal of the Korean institute of surface engineering
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    • v.23 no.4
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    • pp.197-207
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    • 1990
  • Atomic layer epitaxy is a relatively new epitaxial pprocess chracterized by the alternate and separate exposure of a susbstrate surface to the reactants contaning the constituent element of a compound semicoductror. The ideal ALE is expected to provide sevral advantageous as petcts for growing complicated heterostrutures such as relativly easy controls of the layer thinkness down to a monolayer and in forming abrupt heterointerfaces though monolayer self-saturatio of the growth. In addition, since ALE is stongly dependent on the surface reaction, the growth can also be controlled by photo-excitation which provides activation can be energies for each step of the reaction paths. The local growth acceleration by photo-excitation can be exploited for growing several device strures on the same wafer, which provides another important practical advantage. The ALE growth of GaAs has advanced to the point the laser opertion has been achieved from AlGs/GaAs quantun well structures where thee active layers were grown by thermal and Ar-laser assisted ALE. The status of the ALE growth of GaAs and other III-V compounds will be reviewed with respect to the growth saturation behavior and the electrical properties of the grown crystals.

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The Effect of Unprecracked Hydride on the Growth and Carbon Incorporation in GaAs Epilayer on GaAs(100) by Chemical Beam Epitaxy

  • 박성주;노정래;하정숙;이을항
    • Bulletin of the Korean Chemical Society
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    • v.16 no.2
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    • pp.149-153
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    • 1995
  • We have grown GaAs epilayers by chemical beam epitaxy(CBE) using unprecracked hydrides and metal organic compounds via a surface decomposition process. This result shows that unprecracked arsine (AsH3) or monoethylarsine (MEAs) can be used in chemical beam epitaxy(CBE) as a replacement of a precracked AsH3 source in CBE. It was also found that the uptake of carbon impurity in epilayers grown using trimethylgallium(TMG) with unprecracked AsH3 or MEAs was significantly reduced compared to that in epilayers grown by CBE process employing TMG and arsenics produced from precracked hydrides. We propose a surface structural model suggesting that the hydrogen atoms play an important role in the reduction of carbon content in GaAs epilayer. Intermediates like dihydrides from hydride sources were also considered to hinder carbon atoms from being incorporated into the epilayers or to remove other carbon containing species on the surface.

Selective Si Epitaxy for Device Isolation (소자분리를 위한 선택적 실리콘 에피택시)

  • Yang, Jeon Wook;Cho, Kyoung Ik;Park, Sin Chong
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.23 no.6
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    • pp.801-806
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    • 1986
  • The effect of SiH2Cl2 -HCl gas on the growth rate of epitaxial layer is studied. The temperature, pressure and gas mixing ratio of SiH2Cl2 and HCl are varied to study the growth rate dependence and selective Si epitaxy. The P-n junction diode is fabricated on the epitaxial layer and electrical characteristics are examined. Also, using selective Si epitaxy, a possibility of thin dielectric isolation process, that gives an independent isolation width on the mask dimension, is examined.

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GaN Epitaxy with PA-MBE on HF Cleaned Cobalt-silicide Buffer Layer (HF 크리닝 처리한 코발트실리사이드 버퍼층 위에 PA-MBE로 성장시킨 GaN의 에피택시)

  • Ha, Jun-Seok;Chang, Ji-Ho;Song, Oh-Sung
    • Journal of the Korea Academia-Industrial cooperation Society
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    • v.11 no.2
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    • pp.409-413
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    • 2010
  • We fabricated 10 nm-thick cobalt silicide($CoSi_2$) as a buffer layer on a p-type Si(100) substrate to investigate the possibility of GaN epitaxial growth on $CoSi_2/Si(100)$ substrates. We deposited 500 nm-GaN on the cobalt silicide buffer layer at low temperature with a PA-MBE (plasma assisted-molecular beam epitaxy) after the $CoSi_2/Si$ substrates were cleaned by HF solution. An optical microscopy, AFM, TEM, and HR-XRD (high resolution X-ray diffractometer) were employed to determine the GaN epitaxy. For the GaN samples without HF cleaning, they showed no GaN epitaxial growth. For the GaN samples with HF cleaning, they showed $4\;{\mu}m$-thick GaN epitaxial growth due to surface etching of the silicide layers. Through XRD $\omega$-scan of GaN <0002> direction, we confirmed the cyrstallinity of GaN epitaxy is $2.7^{\circ}$ which is comparable with that of sapphire substrate. Our result implied that $CoSi_2/Si(100)$ substrate would be a good buffer and substrate for GaN epitaxial growth.