• 제목/요약/키워드: Optical Set-Up

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Development of the 4th Generation CD Optical Pick-up with Small Thickness (4세대 박형 CD 광학 픽업 개발)

  • 최영석;김성근
    • Journal of the Korean Society for Precision Engineering
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    • v.15 no.3
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    • pp.38-49
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    • 1998
  • The 3rd generation optical pick-up used popularly in resent years is composed of many optical and electronic components such as laser diode, photo diode, beam splitter, objective lens, grating lens, concave lens, collimator lens etc. Therefore, the design of its optical system and its main base which the said optical and electronic components are set on, is complicated and needs high precision. Its assembly and adjustment in the production line is also difficult. This complication and the demand of high precision get its production cost to be high and its reliability to be low. In this paper, the 4th generation optical pick-up is designed and developed, with the hologram device which laser diode. photo diode, beam splitter. and grating lens are integrated in. This optical pick-up reduces the number of points of adjustment by 3, compared with the 3rd generation optical pick-up of which the number of points of adjustment is 6. This optical pickup also decreases by 4 the number of points of W bonding to have bad influence on environmental reliability, decreases by about 10 the number of parts, and establishes about 20% cost-down of material cost, compared with the 3rd generation optical pick-up.

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Effect of spectral drift to coherent optical fiber sensor (가간섭성 광섬유 센서에 대한 주파수 천이도의 영향)

  • Choi, Kyoo-Nam
    • The Journal of the Korea institute of electronic communication sciences
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    • v.11 no.3
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    • pp.277-282
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    • 2016
  • Effect of spectral drift in coherent fiber laser was investigated by injecting optical feedback to Fabry-Perot resonance loop. Er+3 doped fiber laser having unilateral optical feedback loop in Fabry-Perot configuration using two FBGs was fabricated. The optical feedback was found to be effective in linewidth reduction of fiber laser compared to the case without any optical feedback. The linewidth of three fiber lasers using above configuration were measured to be within 3kHz which is resolution-limited performance of self-heterodyne linewidth measurement set-up. The frequency drift measurement using Mach-Zehnder measurement set-up having 200m optical delay-line in one arm showed that the frequency drift rate of optical feedback fiber laser was measured as 300kHz/sec which was better than the case without optical feedback.

Measurement of Color Uniformity of Liquid Crystal Projection Display

  • Ying, Chen;Haifeng, Li;Mo, Shen;Xu, Liu;Shizhe, Shen
    • 한국정보디스플레이학회:학술대회논문집
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    • 2004.08a
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    • pp.483-486
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    • 2004
  • A CCD-based color uniformity measurement system was set up. Through measuring the two-dimensional brightness distributions of three primary colors on the screen, chromaticity coordinate distributions of combination gray can be obtained within a few seconds. This system can be widely used in the production of LCD projection.

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Thed Optimum Optical Geometry for Recording a Full Color Transmission type Holographic Screen of Larged Size

  • Kim, Jai-Soon;Bobrinev, V.I.;Son, Jung-Young;Choi, Yong-Jin;Shin, Sang-Hun
    • Journal of the Optical Society of Korea
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    • v.4 no.1
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    • pp.66-70
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    • 2000
  • The main problem of image projection on a transmission type holographic screen is color sepa-ration. And it can be overcome by using a long narrow slit type diffuser as a source of the object beam when we record the screen. But that screen is not optimized and so needs changing several conditions. To set up the system many complicate things should be taken into accounted so it is very important to analyze the basic structure by simple concepts and calculations. We designed the system so that recording and projection axis coincide in one line and showed that the analysis of the system is very simple. We did it by a 1st order paraxial approximation calculation and it was good enough to describe the system. The photo-emulsion layer shrinks after processing of the hologram. It induced unsatisfactory color matching at the viewing zone. To overcome this effect, we pre-checked the shrinkage rate of an emulsion layer by experiments and modified the recording set up to compensate for the amount of shrinkage.

Comparisons of Object Recognition Performance with 3D Photon Counting & Gray Scale Images

  • Lee, Chung-Ghiu;Moon, In-Kyu
    • Journal of the Optical Society of Korea
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    • v.14 no.4
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    • pp.388-394
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    • 2010
  • In this paper the object recognition performance of a photon counting integral imaging system is quantitatively compared with that of a conventional gray scale imaging system. For 3D imaging of objects with a small number of photons, the elemental image set of a 3D scene is obtained using the integral imaging set up. We assume that the elemental image detection follows a Poisson distribution. Computational geometrical ray back propagation algorithm and parametric maximum likelihood estimator are applied to the photon counting elemental image set in order to reconstruct the original 3D scene. To evaluate the photon counting object recognition performance, the normalized correlation peaks between the reconstructed 3D scenes are calculated for the varied and fixed total number of photons in the reconstructed sectional image changing the total number of image channels in the integral imaging system. It is quantitatively illustrated that the recognition performance of the photon counting integral imaging system can be similar to that of a conventional gray scale imaging system as the number of image viewing channels in the photon counting integral imaging (PCII) system is increased up to the threshold point. Also, we present experiments to find the threshold point on the total number of image channels in the PCII system which can guarantee a comparable recognition performance with a gray scale imaging system. To the best of our knowledge, this is the first report on comparisons of object recognition performance with 3D photon counting & gray scale images.

NEW DIGITAL H$\alpha$ OBSERVATION BY SOLAR FLARE TELESCOPE AT BOAO

  • LEE C.-W.;MOON Y.-J.;PARK Y.D.;JANG B.-H.;KIM KAP-SUNG
    • Journal of The Korean Astronomical Society
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    • v.34 no.2
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    • pp.111-117
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    • 2001
  • Recently, we have set up a new digital CCD camera system, MicroMax YHS-1300 manufactured by Roper Scientific for Ha observation by Solar Flare Telescope at Bohyunsan Optical Astronomy Observatory. It has a 12 bit dynamic range, a pixel number of 1300$\times$1030, a thermoelectric cooler, and an electric shutter. Its readout speed is about 3 frames per second and the dark current is about 0.05 e-/p/s at $-10^{\circ}C$. We have made a system performance test by confirming the system linearity, system gain, and system noise that its specification requires. We have also developed a data acquisition software which connects a digital camera con-troller to a PC and acquires H$\alpha$ images via Microsoft Visual C++ 6.0 under Windows 98. Comparisons of high quality H$\alpha$ images of AR 9169 and AR 9283 obtained from SOFT with the corresponding images from Learmonth Solar Observatory in Australia confirm that our H$\alpha$ digital observational system is performed properly. Finally, we present a set of H$\alpha$ images taken from a two ribbon flare occurred in AR 9283.

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Fabrication of a Single Molecule Detection System and Its Application: Connection between Ensemble and Single Molecule Measurements

  • Park, Mira;Lee, Heung Soon;Kim, DongHo;Song, Nam Woong
    • Journal of Photoscience
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    • v.11 no.32
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    • pp.47-53
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    • 2004
  • A laser scanning fluorescence microscope system has been fabricated for single molecule detection (SMD). Problems associated with the system set-up have been discussed along with proper suggestions. Based on the SMD results obtained by using the apparatus, a statistical method has been suggested to determine the minimum number of required molecules to form a group of uniform average in a selected error range.

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The Development of Beam Rotating Actuator for High Speed Optical Disk Storage (고속 광학기록매체용 다중빔 회전 구동기의 개발)

  • 김병준;김수현;곽윤근
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 1997.10a
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    • pp.1072-1075
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    • 1997
  • To enhance the effective data transfer rate the multi-beam optical disk drive is presented. The Beam rotating actuator is necessary for putting multi-beam on more than one track. Ray tracing was also executed for real system set-up. The Beam Rotating Actuator is made up of piezoelectric material, high stiffness wire hinge and dove prism. The actuator has about 1kHz natural frequency and suitable and suitable operational range. The dynamic equation for the actuator is derived for the control of real system.

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The Development and Performance Analysis of Beam Rotating Actuator for Multi-Beam Disk Drive (다중빔 광디스크용 빔 회전 구동기의 제작과 특성평가)

  • Kim, Byeong-Jun;Kim, Su-Hyeon;Gwak, Yun-Geun
    • Transactions of the Korean Society of Mechanical Engineers A
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    • v.24 no.12
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    • pp.3026-3032
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    • 2000
  • To enhance the effective data transfer rate the multi-beam optical disk drive is presented. The Beam rotating actuator is necessary for putting multi-beam on more than one track. Ray tracing was also executed for real system set-up. The beam Rotating Actuator is made up of piezoelectric material, high stiffness wire hinge and dove prism. The actuator has about 1kHz natural frequency and suitable operational range. The dynamic equation for the actuator is derived for the control real system.

Investigation of compound semiconductor (레이저를 이용한 화합물 반도체 연구)

  • 이승원
    • Proceedings of the Optical Society of Korea Conference
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    • 1990.02a
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    • pp.211-214
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    • 1990
  • Investigation of GaAs/AlGaAs QW carried out by using PL and Absorption spectroscopy. In order to get high resolution (0.76meV) and low noise, proper experimental system was set-up. From measurements, we have deduced the properties of GaAs/AlGaAs QW, such as the residual impurity, well thickness, crystal quality, interface abruptness and well thickness uniformity. Also we can obtain other properties such as sub-band absorption by using Absorption Spectroscopy.

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