• 제목/요약/키워드: rocking wall

검색결과 57건 처리시간 0.028초

Hot-Wal Epitaxy 방법에 의한 ZnSe/GaAs 박막 성장과 특성 (Growth and characterization of ZnSe/GaAs epilayer by hot-wall epitaxy method)

  • 정태수;강창훈;유평렬
    • 한국진공학회지
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    • 제8권3B호
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    • pp.302-307
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    • 1999
  • We have grown a high quality ZnSe(100) epilayer on the GaAs(100) substrate by hot-wall epitaxy method. The FWHM value from double-crystal x-ray diffraction rocking curve and growth rate of the ZnSe epilayer grown under the optimal growth conditions were 195 arcsec and 0.03 $\mu \textrm m$/min, respectively. The $I_2^U$ and $I_2^L$ peaks, which split by strain due to lattice mismatch between substrate and epilayer, were measured from the photoluminescence experiment. And we found that the residual impurities in ZnSe epilayer were concerned with Al or CI elements from the calculated binding energy of donor impurity.

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HWE 방법에 의한 ZnMnTe 단결정 박막의 성장 및 특성연구 (Characterization and Growth of the ZnMnTe epilayers by HWE)

  • 윤만영;박재준;박재규;유영문;최용대
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2001년도 춘계학술대회 논문집 유기절연재료 전자세라믹 방전플라즈마 연구회
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    • pp.208-211
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    • 2001
  • Hot wall epitaxy 법으로 GaAs(100) 기판 위에 $Zn_{1-x}Mn_xTe(0{\leq}x{\leq}1)$ 단결정 박막을 성장하였다. XRD 스펙트럼으로부터 $Zn_{1-x}Mn_xTe$ epilayer들이 전 영역에 걸쳐 zincblende 구조임을 알았다. double crystal rocking curve(DCRC)로부터 격자상수를 계산하고 이훌 이용하여 조성비를 계산하였다. ZnMnTe 단결정 박막의 DCRC 반치폭은 Mn 조성비가 증가함에 따라 급격하게 증가하다가 포화되는 모습을 나타내었다

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저층 조적건물의 내진성능평가 사례 연구 (Case Study of Seismic Evaluation of Low-Rise Masonry Buildings)

  • 엄태성;김찬호;이승제;김진우
    • 한국지진공학회논문집
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    • 제26권1호
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    • pp.1-11
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    • 2022
  • In this study, the seismic performance of a two-story unreinforced masonry (URM) building was assessed following the linear and nonlinear static procedures specified in the seismic evaluation guideline of existing buildings. First, the provisions to assess failure modes and shear strengths of URM walls and wall piers were reviewed. Then, a two-story URM building was assessed by the linear static procedure using m-factors. The results showed that the walls and wall piers with aspect ratios he // (i.e., effective height-to-length ratio) > 1.5 were unsafe due to rocking or toe crushing, whereas the walls with he // ≤ 1.5 and governed by bed-joint sliding mainly were safe. Axial stresses and shear forces acted upon individual masonry walls, and wall piers differed depending on whether the openings were modeled. The masonry building was reevaluated according to the nonlinear static procedure for a more refined assessment. Based on the linear and nonlinear assessment results, considerations of seismic evaluation for low-rise masonry buildings were given with a focus on the effects of openings.

HWE 방법에 의한 $AgGaS_2$/GaAs epilayer 성장과 특성 (Study of characteristics of $AgGaS_2$/GaAs epilayer by hot wall epitaxy)

  • 홍광준;정준우;방진주;진윤미;김소형;여회숙;양해정
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2002년도 제4회 영호남학술대회 논문집
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    • pp.84-91
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    • 2002
  • The stochiometric composition of $AgGaS_2$/GaAs polycrystal source materials for the $AgGaS_2$/GaAs epilayer was prepared from horizontal furnace. From the extrapolation method of X-ray diffraction patterns it was found that the polycrystal $AgGaS_2$/GaAs has tetragonal structure of which lattice constant an and Co were 5.756 $\AA$ and 10.305 $\AA$, respectively. $AgGaS_2$/GaAs epilayer was deposited on throughly etched GaAs(100) substrate from mixed crystal $AgGaS_2$/GaAs by the Hot Wall Epitaxy (HWE) system. The source and substrate temperature were $590^{\circ}C$ and $440^{\circ}C$ respectively. The crystallinity of the grown $AgGaS_2$/GaAs epilayer was investigated by the DCRC (double crystal X-ray diffraction rocking curve). The optical energy gaps were found to be 2.61 eV for $AgGaS_2$/GaAs epilayer at room temperature. The temperature dependence of the photocurrent peak energy is well explained by the Varshni equation, then the constants in the Varshni equation are given by $\alpha=8.695{\times}10^{-4}$ eV/K, and $\beta=332K$. From the photocurrent spectra by illumination of polarized light of the $AgGaS_2$/GaAs epilayer, we have found that crystal field splitting ${\Delta}Cr$ was 0.28 eV at 20 K. From the PL spectra at 20 K, the peaks corresponding to free and bound excitons and a broad emission band due to D-A pairs are identified. The binding energy of the free excitons are determined to be 0.2676 eV and 0.2430 eV and the dissociation energy of the bound excitons to be 0.4695 eV.

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Evaluation of crystallinity and defect on (100) ZnTe/GaAs grown by hot wall epitaxy

  • Kim, Beong-Ju
    • 한국결정성장학회지
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    • 제12권6호
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    • pp.299-303
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    • 2002
  • The relationship of crystallinity between defects distribution with (100) ZnTe/GaAs using HWE growth was investigated by four crystal rocking curve (FCRC) and transmission electron microscopy (TEM). The thickness dependence of crystal quality in ZnTe epilayer was evaluated. The FWHM value shows a strong dependence on ZnTe epilayer thickness. For the films thinner than 6 ${\mu}{\textrm}{m}$, the FWHM value decreases very steeply as the thickness increases. For the films thicker than 6 ${\mu}{\textrm}{m}$, it becomes an almost constant value. At the thickness of 12 $\mu\textrm{m}$ with the smallest value of 66 arcsec. which is the best value so far reported on ZnTe epilayers was obtained. Investigation into the nature and behavior of dislocations with film thickness in (100) ZnTe/(100)GaAs heterostructures grown by Hot Wall Epitaxy (HWE). This film defects range from interface to 0.7 ${\mu}{\textrm}{m}$ thickness was high density, due to the large lattice mismatch and thermal expansion coefficients. The thickness of 0.7~1.8 ${\mu}{\textrm}{m}$ was exists low defect density. In the thicker range than 1.8 ${\mu}{\textrm}{m}$ thickness was measured hardly defects.

주입 위치에 따른 기포와 상변화물질의 유동 상호 작용에 관한 연구 (Study on Flow Interaction between Bubble and Phase Change Material according to Injection Location)

  • 김민혁;지윤영;손동기;고한서
    • 한국가시화정보학회지
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    • 제21권3호
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    • pp.75-84
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    • 2023
  • In this study, we conducted analysis of bubble dynamics and flow of liquid phase change material(PCM) using shadowgraphy and particle image velocimetry(PIV). Characteristics of internal flow varied depending on locations of injection when solid PCM was liquefied from heated vertical wall. When bubbles rose immediately, they exhibited elliptical shape and zigzag trajectory. In contrast, when bubbles rose after merging at the bottom of solid PCM, with equivalent diameter for the inter-wall distance of 0.64 or greater, they showed a jellyfish shape and strong rocking behavior. It was observed by the PIV that the small ellipse bubbles made most strong flow inside the liquid PCM. Furthermore, the flow velocity was highest in the case of front injection, as the directions of temperature gradients and bubble-driven flow were aligned. The results underscore the significant influence of injection location on various characteristics, including bubble size, shape, rising path of bubbles, and internal flow.

Hot-wall epitaxy 방법에 의한 HgCdTe 박막 성장 (Growth of HgCdTe thin film by the hot-wall epitaxy method)

  • 최규상;정태수
    • 한국진공학회지
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    • 제9권4호
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    • pp.406-410
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    • 2000
  • Hot-wall epitaxy 방법으로 GaAs (100) 기판 위에 9 $\mu\textrm{m}$의 CdTe (111)을 완충층으로 성장하고 그 위에 in-situ로 $Hg_{1-x}Cd_x$/Te (MCT)박막을 성장하였다. 성장된 MCT박막의 2결정 x-선 요동곡선의 반치폭 값은 125 arcsec이었으며 표면 형상의 roughness는 10 nm의 작고 깨끗한 면을 나타내었다. 성장된 MCT 박막에 대한 광전류 측정으로부터 최대 peak 파장과 cut off 파장은 각각 1.1050 $\mu\textrm{m}$ (1.1220 eV)와 1.2632 $\mu\textrm{m}$ (0.9815 eV)임을 알았다 이 peak 파장은 광전도체의 intrinsic transition에 기인한 band gap에 대응하는 봉우리이다. 이로부터 MCT 박막은 1.0 $\mu\textrm{m}$에서 1.6 $\mu\textrm{m}$의 근적외선 파장 영역을 감지할 수 있는 광전도체용 검출기로 쓰일 수 있음을 알았다.

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파괴모드를 고려한 비보강 조적벽체의 비선형 해석모델 (Nonlinear Analysis Model Considering Failure Mode of Unreinforced Masonry Wall)

  • 백은림;김정현;이상호;오상훈
    • 한국구조물진단유지관리공학회 논문집
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    • 제18권4호
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    • pp.33-40
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    • 2014
  • 본 연구는 비보강 조적조 건축물의 정밀한 내진성능 평가를 위한 기초 연구로써, 조적벽체의 형상비 및 개구부 유무에 따른 파괴모드를 고려하여 기존의 전단강도 제안식을 비교 평가하고, 이를 반영한 복원력 특성모델을 제안하였다. 개구부가 없는 조적벽체의 전단강도는 국내 기존 연구에서 제안된 강체회전 및 양단부 압축파괴 강도와 FEMA의 미끄러짐 전단강도 중 작은 값을, 개구부가 있는 벽체의 경우 Pier 벽체만을 고려하여 강도를 예측하는 것이 적절한 것으로 평가되었다. 또한 파괴모드를 고려하여 휨 및 전단거동의 복원력 특성 모델을 제시하였으며, 이를 적용하여 비선형 반복가력 해석을 수행한 결과, 강도 및 이력 거동 면에서 실험과 유사한 결과를 얻을 수 있었다.

Hot Wall Epitaxy (HWE)법에 의한 ZnIn2S4 단결정 박막 성장과 열처리 효과 (Growth and Effect of Thermal Annealing for ZnIn2S4 Single Crystal Thin Film by Hot Wall Epitaxy)

  • 박창선;홍광준
    • 한국재료학회지
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    • 제18권6호
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    • pp.318-325
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    • 2008
  • Single crystal $ZnIn_2S_4$ layers were grown on thoroughly etched semi-insulating GaAs(100) substrate at $450^{\circ}C$ with hot wall epitaxy (HWE) system by evaporating $ZnIn_2S_4$ source at $610^{\circ}C$. The crystalline structure of the single crystal thin films was investigated by the photoluminescence (PL) and double crystal X-ray rocking curve (DCRC). The temperature dependence of the energy band gap of the $ZnIn_2S_4$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)=2.9514\;eV-(7.24{\times}10^{-4}\;eV/K)T^2/(T+489\;K)$. After the as-grown $ZnIn_2S_4$ single crystal thin films were annealed in Zn-, S-, and In-atmospheres, the origin of point defects of $ZnIn_2S_4$ single crystal thin films has been investigated by the photoluminescence (PL) at 10 K. The native defects of $V_{Zn}$, $V_S$, $Zn_{int}$, and $S_{int}$ obtained by PL measurements were classified as a donors or acceptors type. And we concluded that the heat-treatment in the S-atmosphere converted $ZnIn_2S_4$ single crystal thin films to an optical p-type. Also, we confirmed that In in $ZnIn_2S_4$/GaAs did not form the native defects because In in $ZnIn_2S_4$ single crystal thin films existed in the form of stable bonds.

Hot Wall Epitaxy (HWE)법에 의한 ZnIn2Se4 단결정 후막 성장과 열처리 효과 (Growth and effect of thermal annealing for ZnIn2Se4 single crystalline thick film by hot wall epitaxy)

  • 홍명석;홍광준
    • 센서학회지
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    • 제17권6호
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    • pp.437-446
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    • 2008
  • Single crystalline ${ZnIn_2}{Se_4}$ layers were grown on thoroughly etched semi-insulating GaAs (100) substrate at $400^{\circ}C$ with hot wall epitaxy (HWE) system by evaporating ${ZnIn_2}{Se_4}$ source at $630^{\circ}C$. The crystalline structure of the single crystalline thick films was investigated by the photoluminescence (PL) and Double crystalline X-ray rocking curve (DCRC). The carrier density and mobility of ${ZnIn_2}{Se_4}$ single crystalline thick films measured from Hall effect by van der Pauw method are $9.41{\times}10^{16}cm^{-3}$ and $292cm^2/V{\cdot}s$ at 293 K, respectively. The temperature dependence of the energy band gap of the ${ZnIn_2}{Se_4}$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)$=1.8622 eV-$(5.23{\times}10^{-4}eV/K)T^2$/(T+775.5 K). After the as-grown ${ZnIn_2}{Se_4}$ single crystalline thick films was annealed in Zn-, Se-, and In-atmospheres, the origin of point defects of ${ZnIn_2}{Se_4}$ single crystalline thick films has been investigated by the photoluminescence (PL) at 10 K. The native defects of $V_{Zn}$, $V_{Se}$, $Zn_{int}$, and $Se_{int}$ obtained by PL measurements were classified as a donors or acceptors type. And we concluded that the heat-treatment in the Se-atmosphere converted ${ZnIn_2}{Se_4}$ single crystalline thick films to an optical p-type. Also, we confirmed that In in ${ZnIn_2}{Se_4}$/GaAs did not form the native defects because In in ${ZnIn_2}{Se_4}$ single crystalline thick films existed in the form of stable bonds.