• Title/Summary/Keyword: 1064 nm

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Quantitative Measurement of Soot concentration by Two-Wavelength Correction of Laser-Induced Incandescence Signals (2파장 보정 Laser-Induced Incandescence 법을 이용한 매연 농도 측정)

  • 정종수
    • Transactions of the Korean Society of Automotive Engineers
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    • v.5 no.3
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    • pp.54-65
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    • 1997
  • To quantify the LII signals from soot particle of flames in diesel engine cylinder, a new method has been proposed for correcting LII signal attenuated by soot particles between the measuring point and the detector. It has been verified by an experiment on a laminar jet ethylene-air diffusion flame. Being proportional to the attenuation, the ratio of LII signal at two different detection wavelengths can be used to correct the measured LIIsignal and obtain the unattenuated LII signal, from which the soot volume fraction in the flame can be estimated. Both the 1064-nm and frequency-doubled 532-nm beams from the Nd : YAG laser are used. Single-shot, one-dimensional(1-D) line images are recorded on the intensified CCD camera, with the rectangular-profile laser beam using 1-mm-diameter pinhole. Two broadband optical interference filters having the center wavelengths of 647 nm and 400 nm respectively and a bandwidth of 10 nm are used. This two-wavelength correction has been applied to the ethylene-air coannular laminar diffusion flame, previously studied on soot formation by the laser extinction method in this laboratory. The results by the LII measurement technique and the conventional laser extinction method at the height of 40 nm above the jet exit agreed well with each other except around outside of the peaks of soot concentration, where the soot concentration was relatively high and resulting attenuation of the LII signal was large. The radial profile shape of soot concentration was not changed a lot, but the absolute value of the soot volume fraction around outside edge changed from 4ppm to 6.5 ppm at r=2.8mm after correction. This means that the attenuation of LII signal was approximately 40% at this point, which is higher than the average attenuation rate of this flame, 10~15%.

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The Optical Design of Probe-type Microscope Objective for Intravital Laser Scanning CARS Microendoscopy

  • Rim, Cheon-Seog
    • Journal of the Optical Society of Korea
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    • v.14 no.4
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    • pp.431-437
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    • 2010
  • A stack of gradient-index (GRIN) rod lenses cannot be used for coherent anti-Stokes Raman scattering (CARS) microendoscopy for insertion to internal organs through a surgical keyhole with minimal invasiveness. That's because GRIN lens has large amount of inherent chromatic aberrations in spite of absolutely requiring a common focus for pump and Stokes beam with each frequency of ${\omega}_p$ and ${\omega}_S$. For this endoscopic purpose, we need to develop a long slender probe-type objective, namely probe-type microscope objective (PMO). In this paper, we introduce the structure, the working principle, and the design techniques of PMO which is composed of a probe-type lens module (PLM) and an adaptor lens module (ALM). PLM is first designed for a long slender type and ALM is successively designed by using several design parameters from PLM for eliminating optical discords between scanning unit and PLM. A combined module is optimized again to eliminate some coupling disparities between PLM and ALM for the best PMO. As a result, we can obtain a long slender PMO with perfectly diffraction-limited performance for pump beam of 817 nm and Stokes beam of 1064 nm.

Simultaneous Detection of Biomolecular Interactions and Surface Topography Using Photonic Force Microscopy

  • Heo, Seung-Jin;Kim, Gi-Beom;Jo, Yong-Hun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2014.02a
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    • pp.402.1-402.1
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    • 2014
  • Photonic force microscopy (PFM) is an optical tweezers-based scanning probe microscopy, which measures the forces in the range of fN to pN. The low stiffness leads proper to measure single molecular interaction. We introduce a novel photonic force microscopy to stably map various chemical properties as well as topographic information, utilizing weak molecular bond between probe and object's surface. First, we installed stable optical tweezers instrument, where an IR laser with 1064 nm wavelength was used as trapping source to reduce damage to biological sample. To manipulate trapped material, electric driven two-axis mirrors were used for x, y directional probe scanning and a piezo stage for z directional probe scanning. For resolution test, probe scans with vertical direction repeatedly at the same lateral position, where the vertical resolution is ~25 nm. To obtain the topography of surface which is etched glass, trapped bead scans 3-dimensionally and measures the contact position in each cycle. To acquire the chemical mapping, we design the DNA oligonucleotide pairs combining as a zipping structure, where one is attached at the surface of bead and other is arranged on surface. We measured the rupture force of molecular bonding to investigate chemical properties on the surface with various loading rate. We expect this system can realize a high-resolution multi-functional imaging technique able to acquire topographic map of objects and to distinguish difference of chemical properties between these objects simultaneously.

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Direct Etching of Polymethyl methacrylate (PMMA) for Microchannels (Polymethyl methacrylate (PMMA)의 마이크로 채널 형성을 위한 레이저의 직접식각)

  • Shin, Sung-Kwon;Choi, Yong-Jin;Lee, Cheon
    • Proceedings of the KIEE Conference
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    • 2007.07a
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    • pp.286-287
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    • 2007
  • 본 논문에서는 최근 유체소자 재료로써 많이 사용되고 있는 polymethyl methacrylate (PMMA)의 레이저 직접식각에 관한 특성을 나타내었다. 식각을 위한 레이저 원으로 기본파가 1064 nm, 반복율이 10 Hz인 Nd:YAG 레이저의 4고조파 성분 ($\lambda$=266 nm)을 사용하였다. X-Y-Z 축으로 이동 가능한 스테이지의 수평 이동속도를 변화시키며, 표면으로 조사되는 펄스 수를 제어하였다. 식각 후 광학현미경으로 식각 단면을 조사하여 식각 깊이와 폭을 측정하였다. 측정된 식각 깊이로부터 식각률을 계산하고, 그 값과 레이저 빔 밀도와의 관계를 알아보았다. 그 결과 시료 표면에 조사되는 레이저 빔 밀도의 로그값과 선형적인 관계를 갖는 것을 확인할 수 있었다. 또한 주사전자현미경을 이용하여 채널 형상 및 채널 내벽을 관찰하였다. 마이크로 채널 내벽에 식각 과정에서 발생한 생성물의 제거를 위해, 레이저 식각과 함께 질소가스 블로잉을 해주었다. 질소 블로잉 압력 1500 torr에서 식각 잔유물이 제거된 내벽을 볼 수 있었다. 실험결과, Nd:YAG 4고조파를 이용하여 PMMA 기판상에 유체 이동을 위한 마이크로 채널을 형성시킬 수 있었다.

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Experimental Study for Removing Artificial Patinas of Bronze Sculpture by Nd:YAG Laser Cleaning System (청동 조형물의 인공 파티나 제거를 위한 Nd:YAG 레이저 적용 실험 연구)

  • Park, Chang-Su;Cho, Nam-Chul
    • Journal of the Korean institute of surface engineering
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    • v.46 no.5
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    • pp.197-207
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    • 2013
  • In the midst of increasing importance of modern cultural assets, especially, most modern bronze objects are exposed to outdoor environment, and as the objects are corroded steadily due to environmental factors the objects lost their original colors on the surface. We performed artificial patinas on the bronze sample per each color of red, black and green and checked cuprite and tenorite which are detected from actual bronze corrosion by analyzing the components. In addition, we applied the existing corrosion removal methods of grinder and sand blaster on a similar sample of bronze mirror per injection pressure and performed comparative analysis on the result with Nd:YAG laser. As a result of Nd:YAG laser cleaning artificial patina from bronze samples, all of the patinas were removed by laser wavelength 1064 nm better than 532 nm. Upon applying to a similar sample of bronze mirror, the artificial patina could be selectively removed from substrates without surface damage when Nd:YAG laser was conducted other than the existing removal method, and so it showed the possibility of application.

A Study of the Diffusion and Rise of Stack Plumes at Coastal Region by Using LIDAR Observation Data

  • Yoon, Ill-Hee
    • International Union of Geodesy and Geophysics Korean Journal of Geophysical Research
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    • v.26 no.1
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    • pp.43-58
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    • 1998
  • The Kwinana Shoreline Fumigation Experiment (KSFE) took place at Fremantle, WA, Australia between January 23 and February 8, 1995. The CSIRO DAR LIDAR measured plume sections from near the Kwinana Power Station (KPS) stacks to up to about 5 km downstream. It also measured boundary layer aerosols and the structure of the boundary layer on some occasions. Both stages A and C of KPS were used as tracers at different times. The heart of the LIDAR system is a Neodymium-doped Yttrium-aluminum-garnet (Nd:YAG) laser operating at a fundamental wavelength of 1064 nm, with harmonics of 532 nm and 355 nm. For these experiments the third harmonic was used because the UV wavelength at 355 nm is eye safe beyond about 50 m. The laser fires a pulse of light 6 ns in duration (about 1.8 m long) and with an energy (at the third harmonic) of about 70 mJ. This pulse subsequently scattered and absorbed by both air molecules and particles in the atmosphere. A small fraction of the laser beam is scattered back to the LIDAR, collected by a telescope and detected by a photo-multiplier tube. The intensity of the signal as a function of time is a measure of the particle concentration as a function of distance along the line of the laser shot. The smoke plume was clearly identifiable in the scans both before and after fumigation in the thermal internal boundary layer (TIBL). Both power station plumes were detected. Over the 9 days of operation, 1,568 plumes scans (214 series) were performed. Essentially all of these will provide instantaneous plume heights and widths, and there are many periods of continuous operation over several hours when it should be possible to compile hourly average plume statistics as well. The results of four days LIDAR observations of the dispersion of smoke plume in the TIBL at a coastal site are presented for the case of stages A and C.

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Multimodal Nonlinear Optical Microscopy for Simultaneous 3-D Label-Free and Immunofluorescence Imaging of Biological Samples

  • Park, Joo Hyun;Lee, Eun-Soo;Lee, Jae Yong;Lee, Eun Seong;Lee, Tae Geol;Kim, Se-Hwa;Lee, Sang-Won
    • Journal of the Optical Society of Korea
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    • v.18 no.5
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    • pp.551-557
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    • 2014
  • In this study, we demonstrated multimodal nonlinear optical (NLO) microscopy integrated simultaneously with two-photon excitation fluorescence (TPEF), second-harmonic generation (SHG), and coherent anti-Stokes Raman scattering (CARS) in order to obtain targeted cellular and label-free images in an immunofluorescence assay of the atherosclerotic aorta from apolipoprotein E-deficient mice. The multimodal NLO microscope used two laser systems: picosecond (ps) and femtosecond (fs) pulsed lasers. A pair of ps-pulsed lights served for CARS (817 nm and 1064 nm) and SHG (817 nm) images; light from the fs-pulsed laser with the center wavelength of 720 nm was incident into the sample to obtain autofluorescence and targeted molecular TPEF images for high efficiency of fluorescence intensity without cross-talk. For multicolor-targeted TPEF imaging, we stained smooth-muscle cells and macrophages with fluorescent dyes (Alexa Fluor 350 and Alexa Fluor 594) for an immunofluorescence assay. Each depth-sectioned image consisted of $512{\times}512$ pixels with a field of view of $250{\times}250{\mu}m^2$, a lateral resolution of $0.4{\mu}m$, and an axial resolution of $1.3{\mu}m$. We obtained composite multicolor images with conventional label-free NLO images and targeted TPEF images in atherosclerotic-plaque samples. Multicolor 3-D imaging of atherosclerotic-plaque structural and functional composition will be helpful for understanding the pathogenesis of cardiovascular disease.

Design of the Large Diameter Faraday Rotator for High-power Laser Systems (고출력 레이저 시스템을 위한 대구경 Faraday Rotator 제작)

  • Hong, Sung-Ki;Seo, Young-Seok;Ko, Kwang-Hoon;Kim, Young-Won;Wee, Sang-Bong;Lim, Chang-Hwan
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.57 no.6
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    • pp.1026-1031
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    • 2008
  • We report on the design and experimental results of a large diameter faraday rotator for the high-power laser system(KLF: Kaeri laser facility) that was completed in late 2007s at Korea Atomic Energy Research Institute. The design involves modelling the magnetic field of cylindrical coil with large diameter(110 mm). Magnetic field generation coil is designed by 6 layers using a rectangular wire with cross-sectional area $3{\times}5[mm^2]$. We obtain an isolation ratio for optical feedback of 35 dB at 1064 nm and magnetic field strengths ${\sim}25kG$. We expect that the design can be widely used optical isolators in high-power laser system.

Distance measurement using pulsed eye-safe laser (펄스형 eye-safe 레이저를 이용한 거리측정)

  • 유병헌;조성학;장원석;김재구;황경현;이동주
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 2004.10a
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    • pp.106-109
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    • 2004
  • In this project, we have developed the eye-safe LRF system of 1.54 ${\mu}{\textrm}{m}$ wavelength using OPO. The maximum measured distance was 3.7km in outdoor experiment. We used Nd:YAG (1064nm) as a laser medium. It was applied BBO to construct the system. We also developed a time-counter for the range finder using a method of TOF (time of flight). The counter-clock used at the time counter was 320MHz making resolution within $\pm$1m. Start and stop signals were detected by two channel systems using PIN and APD. The LRF's repetition rate was 4 times per minute. The energy was measured to be over 9mJ. And, pulse-duration was 23ns. Resolution was $\pm$2m at the distance measurement using a target.

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레이저를 이용한 PDP ITO 전극의 직접 패터닝

  • Gwon, Sang-Jik;Kim, Gwang-Ho;Jeon, Jong-Rok
    • Proceedings of the Korean Society Of Semiconductor Equipment Technology
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    • 2007.06a
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    • pp.94-98
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    • 2007
  • AC PDP에 사용되는 ITO 전극의 공정시간을 단축시키고 생산성을 향상시키기 위해서 $Nd:YVO_4$ laser(${\lambda}=1064\;nm$)를 사용하여 ITO 전극 패턴을 형성하였다. ITO etchant를 사용하여 ITO 전극 패턴을 형성한 샘플과 비교해서 laser를 사용하여 제작한 샘플은 ITO 라인 가장자리에 shoulder와 물결무늬를 형성했다. Q스위치 $Nd:YVO_4$ laser와 갈바노메트릭 스캐닝 시스템을 사용하여 500 mm/s의 스캔속도와 40 kHz의 펄스 반복 율을 기본조건으로 결정했다. PDP 테스트 샘플을 제작하여 방전 테스트를 진행하였다. 사진식각공정을 이용하여 만든 PDP 샘플과 비교해서 laser를 이용하여 제작한 PDP 샘플의 최소 방전유지전압은 더 높게 측정됐다. 이것은 ITO 라인의 shoulder와 물결무늬의 형성과 관련이 있다고 판단된다. 본 실험을 통해 레이저를 이용한 PDP용 ITO 전극막의 직접 패터닝 가능성을 확인할 수 있었다.

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