• Title/Summary/Keyword: 레이저회절 분석장치

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Analysis of Measuring Error for Particle Size Analysis by Laser Diffraction Spectrometer (입자크기분석을 위한 레이저회절 분광계의 측정오차 분석)

  • Ha, Sang-An;Son, Heui-Jeong
    • Journal of Korean Society of Environmental Engineers
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    • v.22 no.4
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    • pp.713-722
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    • 2000
  • This study analysed error of measurement and reproducibility for particle size analysis by the laser diffraction spectrometer. Laser diffraction spectrometers has become a very important method of particle size analysis. This measuring method has the advantage of simple operation, good reproducibility and rapid analysis. A feeding and dispersing system have been developed, which allows mass throughputs between 0.1~23 g/min in flowing air and 1.4~35% in flowing liquid. It has been used as a feeder unit for wet and dry particle size analysis from diffraction patterns. Relevant parameters, such as particle shape, particle size, dispersion, flow rate, concentration were analysed for measuring error. And system parameters of instruments for measurement of dynamic processes, eg, measuring time, focal plane, injection pressure drop and dispersion effect by the ultrasonic and mixing of preliminary treatment, were also discussed.

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An Experimental Device for Understanding the Optical Principles of Image/Diffraction Formation (상(이미지)/회절도형 형성의 광학적 원리를 이해하기 위한 실험장치 제작)

  • Kim, Jin-Gyu;Jeong, Jong-Man;Kim, Mun-Chang;Choi, Joo-Hyoung;Kim, Youn-Joong
    • Applied Microscopy
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    • v.37 no.3
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    • pp.199-208
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    • 2007
  • We have made an optical device to study the wave optics phenomena, such as image and diffraction pattern, constructive and destructive interference, by direct operation of laser beam and optical lenses. It consists of laser beam, goniometer, objective lens, intermediate lens, projection lens, CCD system, and computing system. As a result of the performance test, we were able to magnify samples up to 44 times with the resolution of about $5{\mu}m$. It is expected to help EM users understanding more easily principles of transmission electron microscopy (TEM).

Construction of laser induced grating spectrometer and measurement of thermal grating in $C_3H_8$ flame (레이저 유도 격자 분광장치 제작 및 $C_3H_8$화염에서 열 격자 측정)

  • 박철웅;한재원;이중재;이영우;고동섭
    • Korean Journal of Optics and Photonics
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    • v.12 no.6
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    • pp.446-451
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    • 2001
  • We made a laser induced grating spectrometer(LIGS) and measured the thermal grating signal generated in a $C_3$ $H_{8}$ flame. The thermal grating was formed in the C7Ha flame with two second-harmonic Nd:YAG pulse laser beams, and an LIGS signal was generated by Bragg scattering of a probe laser beam A $r^+.laser(488 nm). We found the modulation period of the signal depends linearly on the spacing of the grating set in the flame. We determined flame temperature by fitting the modulated signal and soot concentration with signal strength. Using this technique, we also obtained temperature profile and soot-particle distribution in a $C_3$ $H_{8}$ flame .e .

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Optical Measurements and Control of Digital Holographic Printing System for 3D Image Reconstruction (3D 영상재현을 위한 디지털 스테레오그램 기록시스템에서의 광특성 측정 및 제어)

  • Kim, Jae-Han;Lee, Gwang-Soon;Hur, Nam-Ho
    • Proceedings of the Korean Society of Broadcast Engineers Conference
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    • 2013.06a
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    • pp.83-84
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    • 2013
  • 홀로그래픽 스테레오그램은, 양안 스테레오스코픽 영상들을 레이저 기준파와 간섭시켜 생성된 홀로그래픽 패턴을 감광매질인 홀로그래픽 필름에 기록한 후, 이를 다시 광학적 회절을 이용하여 3차원 영상으로 재현하는 3차원 디스플레이의 한 방법이다. 본 논문에서는 다시점의 full-color, full-parallax 영상을 디지털 방식의 스테레오그램으로 제작하여 3차원 입체 영상으로 재현하기 위한 기록 시스템에서, 기록 매질인 홀로그래픽 필름 면에서의 영상을 고해상도 영상 센서를 이용하여 직접 획득하고, 이 영상 정보를 분석하여 광축을 제어함으로써, 왜곡없는 최적의 호겔을 형성하여 높은 회절 효율을 갖는 스테레오그램을 제작하기 위한 방법 및 장치에 대한 연구개발 결과를 기술하였다.

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Manufacture of an Acousto-Optical Spectrometer for Radio Astronomical Observations (우주전파관측용 음향광학 전파분광기의 제작)

  • 임인성;최재현;오승엽
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.8 no.1
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    • pp.1-12
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    • 1997
  • The acousto-optical spectrometer as a new type backend of the receiver system for radio astronomical observations is manufactured for radio signal analysis. We studied on the effect of Acousto-Optic and Acousto-Optic devices and designed the optics system. We manufactured the optical mount and the CCD detector for deflected beam and interface card. This acousto-optical spectrometer consisted of a laser, optics, acousto-optic deflector, CCD detector and Interface card. This system use He-Ne laser as a light source and use optics to get parallel beam and to focus the deflected beam. Acousto-optic deflector converts IF signal to ultrasonic wave and deflect the laser beam according to the Bragg deflection. The ultra wide band acousto-optic deflector has 1 GHz bandwidth and a total of 2,048 channel Charge Coupled Device for signal detection. In this study, we discuss the theoretical description on the effect of Acousto-optics, the design of the optics, manufacture of optical mount, CCD detector, interface card and we presented the results of experiment. As a result of measurement, we have 1,000 channels bandwidth from CCD channels.

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Methylene Blue Photodegradation Properties of Anatase/brookite Hybrid TiO2 Photocatalyst Prepared with Different Acid Catalysts (산 촉매에 따른 아나타제/브루카이트 혼성형 TiO2 광촉매의 메틸렌블루 광분해특성)

  • Yun, Seok-Min;Kim, Jinhoon;Jeong, Euigyung;Im, Ji Sun;Lee, Young-Seak
    • Applied Chemistry for Engineering
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    • v.22 no.1
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    • pp.21-25
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    • 2011
  • In this study, anatase/brookite hybrid $TiO_2$ was prepared using different acid catalysts and microwave to improve photodegradation of organic pollutants. The methylene blue photodegradation properties of the prepared photocatalysts with different particle/crystal size and brookite fractions were investigated. Surface characteristics and particle sizes of anatase/brookite hybrid $TiO_2$ were evaluated using scanning electron microscopy (SEM) and laser diffraction particle size analyzer, respectively and crystal structures were investigated with X-ray diffraction (XRD). Methylene blue photodegradation properties were evaluated with UV-vis spectrophotometer. Anatase and anatase/brookite hybrid $TiO_2$ had less than 500 nm size of clusters and the average particle size of $6.66{\sim}6.85{\mu}m$, suggesting that types of acid catalysts did not affect the size. XRD of the prepared $TiO_2$ showed that the photocatalysts had anatase/brookite hybrid crystal structure and applying microwave did not change their crystal structure. Photodegradation of methylene blue with the prepared photocatalyst did not increased proportionally to the fraction of brookite and the crystal size and decreased when brookite fraction and the crystal size increased further. Anatase/brookite hybrid $TiO_2$ with brookite fraction of 9.4% and crystal size of 4.53 nm shows the best photodegradation activity of methylene blue.

산화아연의 박막 또는 나노선의 전기화학적 합성과 자외선 센서의 적용

  • Yun, Sang-Hwa;Lee, Dong-Gyu;Yu, Bong-Yeong
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2011.05a
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    • pp.26.2-26.2
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    • 2011
  • 최근 주목 받고 있는 산화아연(ZnO)은 레이저 다이오드, 가스 센서, 자외선 센서, 투명전극 등으로 다양하게 사용될 수 있어 연구개발이 폭 넓게 이루어지고 있는 상황이다. 특히, 3.3 eV의 direct bandgap 에너지를 가지고 있는 ZnO은 현재 자외선센서로 많이 적용되고 있는 물질인 GaN계열을 대체할 수 있는 유망한 물질로 주목 받고 있다. 공기중의 산소나 수분의 표면반응에 의한 자외선 측정을 하는 ZnO을 나노선으로 만들게 되면, 표면대비 부피비가 박막에 비해 급격히 증가하기 때문에 민감도가 커지고 반응시간이 짧아지게 된다. 본 연구에서는 자외선센서의 민감도와 반응성을 향상시키기 위해 전기화학적 합성법을 통해 ZnO의 박막과 나노선을 제조하였다. 사진공정을 통해 3 ${\mu}m$의 간격을 가진 금(Au) 전극을 만든 후, 전기화학적 합성법을 통해 아연이온이 포함된 용액에서 정전류를 흘려보내 아연 또는 ZnO을 증착시킬 수 있었다. 첫 번째로 ZnO을 양쪽 Au 전극에서 동시에 증착하여 두 박막이 접합하였고, 두 번째는 100nm의 지름을 가진 Ni 나노선를 전극 양쪽에서 자석을 통해 자기장을 형성해 정렬시키고 ZnO을 Au 전극과 Ni 나노선에 증착한 후, Ni 나노선를 산화시킴으로써, ZnO 나노구조를 형성하였다. 세 번째로는 Au 전극 양쪽에 아연을 전기화학적 합성을 하여 박막으로 증착하고 고온에서 산화과정을 통해 100 nm 이하의 지름을 가진 ZnO 나노선를 형성하였다. 이렇게 만들어진 세가지 구조의 ZnO의 나노구조와 결정성은 주사전자현미경과 X선 회절 분석기를 통해 측정하였으며, 자외선에 대한 민감도와 반응성은 365 nm의 파장을 가진 자외선발생기와 소스미터장치를 통해 측정하였다. 박막에서 100 nm 이하의 지름을 가진 ZnO 나노선로 갈 수록 자외선에 대한 민감도와 반응성이 향상되었다.

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Luminescence Characteristics of (Y0.85-xYb0.15)3Ga5O12:Er3+x Phosphors ((Y0.85-xYb0.15)3Ga5O12:Er3+x 형광체의 형광특성)

  • Chung, Jong Won;Yi, Soung Soo
    • New Physics: Sae Mulli
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    • v.68 no.12
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    • pp.1308-1314
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    • 2018
  • $Er^{3+}$ and $Yb^{3+}$ co-doped $Y_3Ga_5O_{12}$ polycrystalline powders were prepared by using a solid-state reaction method, and their crystallinities were measured using X-ray diffraction. According to the results of X-ray diffraction, the powders showed a polycrystalline tetragonal structure. The photoluminescence and the upconversion luminescence properties of the $(Y_{0.85-x}Yb_{0.15})_3Ga_5O_{12}:Er^{3+}_x$ (x = 0.03, 0.06, 0.09, 0.12 and 0.15) phosphors were investigated in detail. Green and red upconversion emissions were observed for the phosphors excited by 980 nm radiation from a semiconductor laser. The powders exhibited strong green and weak red upconversion emission peaks at 553 and 660 nm, respectively. Also, their upconversion processes were explained using an energy-diagram analysis and the strongest upconversion intensity was emitted by the powder with a 0.12 mol $Er^{3+}$ ion concentration.

Study on the Composition and Crystallization of TiNi Thin Films Fabricated by Pulsed Laser Deposition in Ambient Ar Gas (Ar가스 분위기에서 PLD방법으로 제작된 TiNi박막의 조성 및 결정성에 관한 연구)

  • Cha, J.O.;Shin, C.H.;Yeo, S.J.;Ahn, J.S.;Nam, T.H.
    • Journal of the Korean Vacuum Society
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    • v.16 no.2
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    • pp.116-121
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    • 2007
  • TiNi shape memory alloy(SMA) was fabricated by PLD(plused laser deposition) using equiatomic TiNi target. Composition and crystallization of TiNi thin films which were fabricated in ambient Ar gas(200m Torr)and vacuum($5{\times}10^{-6}\;Torr$) were investigated. Composition of TiNi thin films was characterized by energy-dispersive X-ray spectrometry (EDXS) and crystallization was confirmed by X-ray diffraction (XRD). The composition of films depends on the distance between target and substrate but does not sensitively depend on the substrate temperature. It is found that the composition of films can be easily controlled when substrate is placed inside plume in ambient Ar gas. It is also found that the in situ crystallization temperature ($ca.\;400^{\circ}C$) in ambient Ar gas is lowered in comparison with that of TiNi film prepared under vacuum. The low crystallization temperature in ambient Ar gas makes it possible to prepare the crystalline TiNi thin film without contamination.