• 제목/요약/키워드: Diffraction order

검색결과 968건 처리시간 0.027초

6H-SiC 에피층 성장과 결정구조 해석 (6H-SiC epitaxial growth and crystal structure analysis)

  • Kook-Sang Park;Ky-Am Lee
    • 한국결정성장학회지
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    • 제7권2호
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    • pp.197-206
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    • 1997
  • 6H-SiC 위에 SiC 에피층이 화학 기상 증착(CVD)에 의하여 성장되었다. 성장된 SiC 에피층의 결정구조는 X-선 회절과 Raman 분광을 사용하여 조사되었으며, 이 에피층은 6H-SiC로서 성장되었음을 확인하였다. 수정된 Lely법으로 성장된 한 SiC 결정 분말의 결정구조를 확인하기 위하여 전형적인 SiC polytype들의 X-선 회절상을 계산하였으며, 측정된 X-선 회절상과 비교하여 이 SiC 결정에는 15R-SiC가 약간 혼재되어 있음을 확인하였다.

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한국 해안에 퇴적된 연약지반의 점토광물의 종류와 분포 (Clay Minerals and Their Distribution in the Soft Ground Deposited along the Coastline)

  • 김상규;임희대;문성권
    • 한국지반공학회지:지반
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    • 제14권6호
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    • pp.73-80
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    • 1998
  • 한국연안에 퇴적된 연약지반에 존재하는 점토광물을 식별하기 위해 여러 위치에서 14개의 시료를 채취하고 X-ray 회절분석을 수행하였다. 연약지반에는 여러 가지 점토광물이 혼합된 상태로 존재하고 halloysite는 존재하지 않는다는 것을 이 분석으로부터 알게 되었다. 지역적인 분포특징을 보면, 서해안과 남해안에서는 kaolinite와 illite가 발견되었으며, montmorillonite는 서해안에서만 존재하였다. 이러한 특징은 그 지역의 지질과 관련시켜 설명될 수 있다. 흙의 물리적 시험으로부터 얻은 활성도는 X-ray 회절분석으로부터 결정된 점토광물의 활성도와 일치성을 보이지 않는다.

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균질기를 이용한 에폭시-층상 실리케이트 나노콤포지트 분산 특성 (Dispersion Properties of Epoxy-layered Silicate Nanocomposites Using Homogenizer)

  • 이상극;박재준
    • 한국전기전자재료학회논문지
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    • 제26권2호
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    • pp.126-133
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    • 2013
  • This paper presents a study on the dispersion effect of the X-Ray diffraction, glass transition and DMA properties of organic modifier clay/epoxy nanocomposites produced in a homogenizer. Several experiments were conducted including different types of dispersion condition with varying processing conditions such as homogenizer rotor speed and applied time of homogenizer. The effects of these variables on the dispersion properties of nanocomposites were then studied. In order to fully understand the experimental results, a X-ray diffraction, DSC and DMA were used to investigate the effect of above mentioned variables on microstructure and intercalation/exfoliation of organic modifier clay/epoxy nanocomposites. The results from this work could be used to determine the best processing condition to obtain appropriate levels of d-spacing, glasss transition temperature and storage modulus in organic modifier clay/epoxy nanocomposites.

Numerical Study on Wave Run-up of a Circular Cylinder with Various Diffraction Parameters and Body Drafts

  • Jeong, Ho-Jin;Koo, Weoncheol;Kim, Sung-Jae
    • 한국해양공학회지
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    • 제34권4호
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    • pp.245-252
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    • 2020
  • Wave run-up is an important phenomenon that should be considered in ocean structure design. In this study, the wave run-up of a surface-piercing circular cylinder was calculated in the time domain using the three-dimensional linear and fully nonlinear numerical wave tank (NWT) techniques. The NWT was based on the boundary element method and the mixed Eulerian and Lagrangian method. Stokes second-order waves were applied to evaluate the effect of the nonlinear waves on wave run-up, and an artificial damping zone was adopted to reduce the amount of reflected and re-reflected waves from the sidewall of the NWT. Parametric studies were conducted to determine the effect of wavelength, wave steepness, and the draft of the cylinder on the wave run-up of the cylinder. The maximum wave run-up value occurred at 0°, which was in front of the cylinder, and the minimum value occurred near the circumferential angle of 135°. As the diffraction parameter increased, the wave run-up increased up to 1.7 times the wave height. Furthermore, the wave run-up was 4% higher than the linear wave when the wave steepness was 1/35. In particular, the crest height of the wave run-up increased by 8%.

피코초 레이저를 이용한 회절 격자 금형 개발 (Practical application of picosecond laser micro-machining to the direct fabrication of a diffraction grating mold)

  • 노지환;이제훈;손현기;서정;신동식
    • 한국정밀공학회:학술대회논문집
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    • 한국정밀공학회 2006년도 춘계학술대회 논문집
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    • pp.487-488
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    • 2006
  • Picosecond (ps) laser micro-machining has emerged as an attractive method of fabricating high-precision microstructures, especially in metals. In this paper, a metallic mold for diffraction gratings is fabricated with a mode-locked 12 Ps $Nd:YVO_4$ laser. Laser pulses with a wavelength of 355nm are irradiated on the surface of NOK 80, a mold material, to generate line patterns. In order to minimize the line width, laser power is set just above the ablation threshold of NOK 80. Results show that the spectrum from the fabricated mold is good enough for some industrial application.

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Effect of the Photosensitizer on the Photo refractive Effect Using a Low $T_g$ Sol-Gel Glass

  • Choi, Dong-Hoon;Jun, Woong-Gi;Oh, Kwang-Yong;Yoon, Han-Na;Kim, Jae-Hong
    • Macromolecular Research
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    • 제11권4호
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    • pp.250-255
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    • 2003
  • We prepared the photorefractive sol-gel glass based on organic-inorganic hybrid materials containing a charge transporting molecule, second-order nonlinear optical (NLO) chromophore, photosensitizer, and plasticizer. Carbazole and 2-{ 4-[(2-hydroxy-ethyl)-methyl-amino]-benzylidene}-malononitrile were reacted with isocyanato-triethoxy silane and the functionalized silanes were employed to fabricate the efficient photorefractive media induding 2,4,7-trinitrot1uorenone (TNF) to form a charge transfer complex. The prepared sol-gel glass samples showed a large net gain coefficient and high diffraction efficiency at a certain composition. As the concentration of photosensitizer increased, the photorefractive properties were enhanced due to an increment of charge carrier density. Dynamic behavior of the diffraction efficiency was also investigated with the concentration of the photosensitizer.

Design and Analysis of a 10× Optical Zoom System for an LWIR Camera

  • Ok, Chang-Min;Park, Sung-Chan
    • Journal of the Optical Society of Korea
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    • 제18권5호
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    • pp.574-581
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    • 2014
  • This paper presents the design and evaluation of the optical zoom system for an LWIR camera. The 12.8operating wavelength range of this system is from $7.7{\mu}m$ to $12.8{\mu}m$. Through a paraxial design and optimization process, we have obtained the extended four-group inner-focus zoom system with focal lengths of 10 to 100 mm, which consists of the six lenses including four aspheric surfaces and two diffractive surfaces. The diffractive lenses were used to balance the higher-order aberrations, and its diffraction properties were evaluated by scalar diffraction theory. We have calculated the polychromatic integrated diffraction efficiency and the MTF drop generated by background noise. The f-number of the zoom system is F/1.4 at all positions. Fields of view are given by $51.28^{\circ}{\times}38.46^{\circ}$ at wide field and $5.50^{\circ}{\times}4.12^{\circ}$ at narrow field positions. In conclusion, this design procedure results in a $10{\times}$ compact zoom lens system useful for an LWIR camera.

EBSD 기법을 이용한 Gamma TiAl의 마이크로 조직파괴에 관한 연구 (A Study on Gamma TiAl Micro-structural Fracture with EBSD Technique)

  • 김윤해;우병훈;배창원;배성열;;문경만
    • Journal of Advanced Marine Engineering and Technology
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    • 제31권4호
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    • pp.377-384
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    • 2007
  • A backscatter Kikuchi diffraction attachment to an SEM enables the convenient investigation of grain orientations on bulk or micro surface. Their relation to micro structural features gives insight into many aspects of anisotropic materials properties. In micro area such as Micro Electro Mechanical Systems(MEMS) devices is required in order to improve understanding of how they may be expected to perform upon the micro scale. Electro Back Scatter Diffraction (EBSD) helps us to find uniform area as MEMS material. The ${\gamma}-TiAl$ has two different lamellar structures ${\gamma}/{\alpha}2-Ti_3Al$ phase which have shows $\{111\}{\gamma}//\{0001\}{\alpha}2$ plane indexing. The micro size testing specimen was successfully made by this structural relation. Interlamellar structure specimen averagely show $20{\sim}25%$ lower fracture toughness value compare with translamellar specimens Moreover micro fracture surface and micro crack progress were observed.

2-Dimensional Holographic Grating Formation in Chalcogenide Thin Films

  • Lee, Jung-Tae;Yeo, Choel-Ho;Chung, Hong-Bay
    • Transactions on Electrical and Electronic Materials
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    • 제5권1호
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    • pp.34-37
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    • 2004
  • Amorphous chalcogenide thin films, especially a-(Se, S) based films, exhibit a number of photo-induced phenomena. In this study, we make the As$\_$40/Ge$\_$10/Se$\_$15/S$\_$35//Ag thin film and then we measure the holographic diffraction efficiency according to thickness of Ag. And we form the two-dimensional holographic grating. At first, we formed one-dimensional grating and then we form two-dimensional grating by rotate the sample. We found out the most suitable thickness of Ag and in case of As$\_$40/Ge$\_$10/Se$\_$15/S$\_$35//Ag(600${\AA}$), the diffraction efficiency was more higher than other samples. The holographic grating was formed by He-Ne laser(λ=632.8nm). The intensity of incident beam was 2.5mW and incident angle was 20$^{\circ}$. We confirm. the two-dimensional holographic grating by the pattern of diffracted beam and AFM(Atomic Force Microscope) image. We perform the etching process using by 0.26N NaOH in order to confirm clearly two-dimensional grating.

(Ba1-xCax)(Ti0.85Zr0.12Sn0.03)O3계 세라믹스의 미세구조 및 유전 특성 (Microstructure and Dielectric Properties of (Ba1-xCax)(Ti0.85Zr0.12Sn0.03)O3 Ceramics)

  • 신상훈;류주현;신동찬
    • 한국전기전자재료학회논문지
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    • 제27권12호
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    • pp.797-802
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    • 2014
  • In this study, in order to develop the capacitor composition ceramics with the good dielectric properties, $(Ba_{1-x}Ca_x)(Ti_{0.85}Zr_{0.12}Sn_{0.03})O_3$ (abbreviated as BCTZ) ceramics were prepared by the conventional solid-state reaction method. The effects of Ca substitution on the microstructure and dielectric properties was investigated. The X-ray diffraction patterns demonstrated that all the specimens showed perovskite phase, and secondary phases are indicated in the measurement range of X-ray diffraction. Also, all the specimens indicated an rhombohedron phase structure. It was identified from the X-ray diffraction patterns that the secondary phase formed in grain boundaries and then decreased the dielectric properties. For all the specimens, observed one peak was tetragonal cubic phase transition temperature($T_c$), which is located in the vicinity of room temperature.