• Title/Summary/Keyword: Optical lens

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Development of diameter 450 mm Cassegrain tlne collimator (직경 450 mm Cassegrain 형태 시준장치의 제작)

  • 양호순;이재협;이윤우;이인원;김종운;김도형
    • Korean Journal of Optics and Photonics
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    • v.15 no.3
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    • pp.241-247
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    • 2004
  • The collimator is necessary for the assembly and evaluation of high resolution satellite telescope. Traditionally, the off-axis paraboloid has been used as a collimator. However, it has some disadvantages in that it can suffer from air turbulence when the focal length of a collimator is long, which may result in some error in the measurement. In contrast, since the Cassegrain type collimator folds the beam, it occupies smaller space compared to the off-axis paraboloid for the same focal length. This can reduce the air turbulence, which can improve the measurement accuracy. In this paper, we explain the process of design and manufacturing of a diameter 450 mm Cassegrain type collimator, to evaluate the diameter 300 mm satellite telescope. After assembly of primary and secondary mirrors, the final wavefront error of the collimator was 0.07λ(λ=633 nm), which is the diffraction limit.

Effects of storing defocused Fourier plane holograms in three-dimensional holographic disk memories (디스크형 3차원 홀로그래피 메모리에서 비초점 Fourier 면 홀로그램의 저장 효과)

  • 장주석;신동학
    • Korean Journal of Optics and Photonics
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    • v.12 no.1
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    • pp.61-66
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    • 2001
  • Defocused Fourier plane holograms are stored in disk-type holographic memories where thin recording media are used, the areal storage density per hologram and the intensity uniformity of the signal beam at the recording plane are studied. As the pixel pitch of the spatial light modulator that represents binary data increases, the storage density per hologram increases if exact Fourier holograms are stored. When defocused Fourier plane holograms are stored, however, we show that there exists an optimal pixel pitch that maximizes the area storage density per hologram in general, to increase the areal storage density per hologram, f/# of the Fourier transform lens that focuses the data image should be as small as possible. In this case, not only the intensity distribution at the recording plane but also the recording area becomes very sensitive to the degree of defocusing. Therefore, even if the exact Fourier plane holograms are stored, the defocusing effect owing to the medium thickness should be taken into account to achieve the maximal areal storage density per hologram.logram.

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Testing of a Convex Aspheric Secondary Mirror for the Cassegrain Telescope (카세그레인 망원경의 볼록비구면 반사경 파면오차 측정)

  • Kim, Goeun;Rhee, Hyug-Gyo;Yang, Ho-Soon
    • Korean Journal of Optics and Photonics
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    • v.28 no.6
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    • pp.290-294
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    • 2017
  • The Cassegrain telescope consists of a primary concave mirror and a secondary convex mirror. In the case of a secondary mirror, it is more difficult to test wavefront error than for a primary mirror, because it reflects the entire testing beam, as it is convex in shape. In this paper we tested the wavefront error of a complex aspheric convex secondary mirror by using the Simpson-Oland-Meckel Hindle test. To separate the systematic errors, such as fabrication error and alignment error of a meniscus lens, we adopted the QN absolute test (pixel-based absolute test using the quasi-Newton method) as well. Finally, we compared the measured result with that of an ASI (Aspheric Stitching Interferometer) made by the QED company, which resulted in an rms difference of only 2.5 nm, showing a similar shape of astigmatism aberration.

Scanning Acoustic Microsope System Using 200MHZ ZnO Transducer (ZnO를 이용한 초음파 현미경의 제작과 평가)

  • Jang, Ji-Won;Do, Si-Hong;Lee, Jong-Gyu
    • Journal of the Korean Society of Fisheries and Ocean Technology
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    • v.25 no.4
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    • pp.200-208
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    • 1989
  • To the purpose of preparation for investigating aspect of material that not revealed by the light microscope and extending our knowledge in applicable field, a scanning acoustic microscope system of 200MHz was organized and appraised its performance with experiments. Professor N.CHUBACHI in Tohoku University in Sendai, Japan provided the ZnO transducer with lens. The system for transmitting and receiving ultrasonic pulses of 200nsec was organized with a rectangular audio wave generator for modulation of 200MHz carrier wave, gating system for transmitting and receiving, mixer for converting intermediate frequency, a directional coupler, ZnO transducer, radio frequency amplifiers. detecter and personal computer. The Scanning system was driven in micro steps with three stepping motors in the direction of x, y and z axes. The system was a reflecting type scanning acoustic microscope and the operation program processed graphics data from receiving echo intensities. Photograph of fish scale obtained by optical microscope was compared with its image by the scanning acoustic microscope organized here. The result was satisfiable.

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The Need for Change of Korean Optician(optometrist) System (안경사제도의 변화 필요성에 대하여)

  • Seo, Jae-Myoung;Kim, Jae-Do;Kim, Heung-Soo;Shim, Hyun-Suk;Kim, Sang-Hyun
    • Journal of Korean Ophthalmic Optics Society
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    • v.20 no.4
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    • pp.527-536
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    • 2015
  • Purpose: In this paper, we have dealt with problems and improvement of korean optician system. Methods: Using the relevant material of korean optician system and international optometrist system, provides the theoretical basis of the need for regulatory changes optician. Results: The people with refractive errors are increasing, 67% of refractive error test is made from optical shop and korean optician are sufficient trained, many opticians are in charge of the refractive error test at the ophthalmic hospital. We have confirmed that current law does not reflect adequately the nature of optician's work. Conclusions: Since current capacity of the Korean opticians and education system ready to provide health services for people, therefore an korean optician must redefine the law to fit the reality.

Fabrication of Three-Dimensional Curved Microstructures by Two-Photon Polymerization Employing Multi-Exposure Voxel Matrix Scanning Method (다중조사 복셀 매트릭스 스캐닝법을 이용한 이광자 중합에 의한 마이크로 3차원 곡면형상 제작)

  • Lim, Tae-Woo;Park, Sang-Hu;Yang, Dong-Yol;Kong, Hong-Jin;Lee, Kwang-Sup
    • Polymer(Korea)
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    • v.29 no.4
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    • pp.418-421
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    • 2005
  • Three-dimensional (3D) microfabrication process using two-photon polymerization (TPP) is developed to fabricate the curved microstructures in a layer, which can be applied potentially to optical MEMS, nano/micro-devices, etc. A 3D curved structure can be expressed using the same height-contours that are defined by symbolic colors which consist of 14 colors. Then, the designed bitmap figure is transformed into a multi-exposure voxel matrix (MVM). In this work a multi-exposure voxel matrix scanning method is used to generate various heights of voxels according to each laser exposure time that is assigned to the symbolic colors. An objective lens with a numerical aperture of 1.25 is employed to enlarge the variation of a voxel height in the range of 1.2 to 6.4 um which can be controlled easily using the various exposure time. Though this work some 3D curved micro-shapes are fabricated directly to demonstrate the usefulness of the process without a laminating process that is generally required in a micro-stereolithography process.

LED application VLC information network system configuration research (LED를 응용한 VLC 정보 네트워크 시스템 구성 연구)

  • lee, Jun-myung;Jang, Tae-su;Kang, Hyng-kil;Kim, Yong-Kab
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2012.10a
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    • pp.13-14
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    • 2012
  • Than fluorescent lamps or light bulbs, long life, small power consumption and to the development of modern technology, LED (Light Emitting Diode) devices have the advantage of easy control. For these reasons, using the LED device, lighting has been widely used. LED using optical fiber technology using LED lighting technology with the development of wireless communication technology is attracting attention again. Using LED lights this study analyzed the performance of the technology transfer and implementation of the information transmission system of the visible light communication using LED lighting of the White Visible Light Communication (VLC) based PC module transmitter and receiver modules. Has made a system that can transmit information more than the value of the initial distance ~ 50cm, depending on the presence or absence of the lens, in order to increase the efficiency of the LED modules with different efficiencies that could confirm the performance of the implementation of the research, analysis, and application methods. and about the possibility that you want to check.

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Beach Profile Estimation Using a Photogrammetry (사진측정법을 이용한 해빈단면의 추정)

  • Kim, Baeck-Oon;Park, Yong-Ahn;Oh, Im-Sang;Khim, Boo-Keun;Choi, Kyung-Sik
    • The Sea:JOURNAL OF THE KOREAN SOCIETY OF OCEANOGRAPHY
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    • v.3 no.4
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    • pp.228-233
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    • 1998
  • This study presents a close-range photogrammetry that is applicable to beach profile estimation using a non-metric camera. Based on the analysis of oblique video image in which the video camera was installed on a horizontal plane and the field of view was fixed, a new equation to analyze a photograph was developed considering the following aspects: (1) camera is allowed to be rotated about its optical axis and (2) a simple error model is adopted to correct lens distortion and other systematic errors associated with the non-metric camera, which improves accuracy of non-metric imageries. To test the modified technique, photographs of the beach were taken near the Donghae City in February, 1998. In addition, beach profiles were surveyed with conventional dumpy level and surveying staff. RMS error between the estimated and measured beach profiles is less than 10 cm in elevation.

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A Study on the PZT Application for Spacecraft Components under Space Environment (우주환경하의 위성부품용 압전진동자 활용에 관한 연구)

  • Lee, Sang-Hoon;Moon, Guee-Won;Yoo, Seong-Yeon
    • Journal of the Korean Vacuum Society
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    • v.21 no.6
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    • pp.287-294
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    • 2012
  • In the high vacuum condition of the space, outgassing from any assembly of satellite can contaminate satellites, especially second surface mirror and optical lens, it cause satellite to fail in own missions. Therefore, all unit shall be check for compatibility with vacuum using CVCM (Collected Volatile Condensable Material) and TML (Total Mass Loss) in advance. CVCM and TML of the PZT-5 piezoelectric ceramic vibrator has less than 0.1% and 1.0% respectively. Also, it has less than 500 $ng/cm^2/hr$ of Thermoelectric Quartz Crystal Microbalance for vacuum bake-out test using high temperature(more than $80^{\circ}C$) and high vacuum (less than $5.0{\times}10^{-3}$ Pa). Thus, piezoelectric ceramic vibrator may be employed in the vacuum environments. Finally, it can be confirmed that the characteristics change of the piezoelectric ceramic vibrator is less than 1% under vacuum environments.

Characteristics of the Nd:YAG laser with stimulated brillouin scattering phase conjugate mirror (유도 브릴루앙 산란 위상공액 거울을 이용한 Nd:YAG 레이저 발진기의 출력특성)

  • 이동원;이성구;박승현;공홍진
    • Korean Journal of Optics and Photonics
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    • v.13 no.6
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    • pp.548-553
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    • 2002
  • We have investigated the output characteristics of a Nd:YAG oscillator with a Stimulated Brillouin Scattering phase conjugation mirror (SBS-PCM). FC-75 is used as an SBS gain medium and Cr:YAG (T=50%) as a Q-switcher. The SBS-PCM consists of an SBS-cell and a simple plano-convex focusing lens system. For the case of not using a Q-switcher, an SBS-cell doesn't work as a phase conjugation mirror. For the case of using a Q-switcher, the energy characteristics remains nearly the same whether using the SBS-cell or not using it. The pulse width is reduced from 50 ns to 40 ns by an SBS-PCM. When the SBS-cell is used with a Q- switcher, the SBS-cell works very well as a phase conjugation mirror and its beam-profile is improved dramatically. And in order to explain the progression of beam-profile, we propose a simple model based on the nonlinear reflectivity of the SBS-PCM, whose reflectivity is dependent on the pumping intensity at the focal plane.