• Title/Summary/Keyword: 결상

Search Result 110, Processing Time 0.025 seconds

Design and fabrication of a zoom optics having 20 magnification range for mid-IR(3.7-4.8$\mu$m) FLIR system (3.7-4.8$\mu$m 파장대역 FLIR 시스템을 위한 20:1 줌 렌즈 광학계 설계 및 제작)

  • 김현숙;김창우;홍석민
    • Korean Journal of Optics and Photonics
    • /
    • v.10 no.6
    • /
    • pp.462-467
    • /
    • 1999
  • This paper describes the design and fabrication of mid-IR $(3.7-4.8{\mu}m)$ zoom optics which is used for FUR (Forward Looking Infra-Red) system with 320 $\times$ 240 focal plane arrays. The zoom optics has 20 magnification range and maximun 40$^{\circ}$$\times$30$^{\circ}$ of super wide field of view. The locus of zoom is almost linear, which gives easy access of mechanical and electro-mechanical design. The on-axis MTF of zoom optics has been measured and it shows diffraction limited optical performance. For example, it gives 0.692 at 24 cycles/mm at highest magnification, and 7.6 cycles/mradof resolving power is achieved with the operation of attached micro-scanning system.system.

  • PDF

The effect of phase modulation on the central peak intensity in an optical system (광학계의 위상 변조 조건에 따른 중심 강도 변화)

  • 이영철;정창섭;박성종;이윤우
    • Korean Journal of Optics and Photonics
    • /
    • v.11 no.2
    • /
    • pp.67-72
    • /
    • 2000
  • A lot of varIOUS studies are taking advantage of annular masks or various pupil filters to design optical systems such as a digital versatile disc (DVD) pick up head and precise scanning microscopy that have the superresolution beyond the diffraction limit. We considered both annular mask and pupil filter for the superresolution system. Since image quality is a function of annular width, position and modulation amount, we computel'lzed the optimized condition for the phase modulation and mvestigated the variation of lhe center peak: intensity for the phase modulated system From tills result, we were able to detenrune the best conditions for the annular apodizer, wluch give the maximum value of the center peak intensity_ We made especially sure that the phase modulated system have an excellent compensation for spherical aberration as it lllcreases. eases.

  • PDF

Fringe Sensitivity of Projection Moire Topography Due to Position of Light Source and Object Distance According to Grating Periods (영사식 무아레 토포그래피에서 격자 주기에 따른 물체거리와 광원의 위치에 대한 무늬 민감도 변화)

  • Oh, Hyun Seock;Ju, Yun Jae;Jo, Jae Heung
    • Korean Journal of Optics and Photonics
    • /
    • v.27 no.2
    • /
    • pp.67-72
    • /
    • 2016
  • In projection moire topography, the investigation of fringe sensitivity, which means the change rate of fringe order according to object height, is important and necessary to reduce the measurement error of the shape of an object. Using the fringe sensitivity, the determination of the absolute orders of moire fringes can be performed very easily and rapidly. The important parameters in the determination of absolute orders of fringes are the positions of light source and object, and the grating period in projection moire topography. Among these parameters, the fringe sensitivity due to the transverse motion of the light source and the longitudinal motion of the object according to grating periods are analyzed and compared. As a result, whereas the fringe sensitivity in the transverse-motion method increases linearly and gradually as the distance between light source and imaging sensor increases, the fringe sensitivity due to the longitudinal-motion method decreases dramatically as the distance between imaging lens and object increases. In these methods, the fringe sensitivity and its change increase as the grating period increases.

Non-imaging Optical Design of a Measurement Probe for LCD Display Used in a Color Analyzer (LCD 디스플레이용 색채계 렌즈에 관한 비결상 광학설계)

  • Rim, Cheon-Seog
    • Korean Journal of Optics and Photonics
    • /
    • v.22 no.5
    • /
    • pp.239-244
    • /
    • 2011
  • We introduce Gaussian (or paraxial) optics that can be successfully applied to design, for use in a color analyzer, a non-imaging optical system on a measurement probe for LCD display. The color analyzer is used to decompose colored lights leaving from some measurement area on the LCD display to red, green, and blue. The color analyzer must include a condenser lens whose purpose is to gather colored lights to illuminate a small area on the sensor. In order to satisfy a reduction ratio between the measurement area and the sensing area with a non-imaging condition, a condenser lens is analytically treated by means of Gaussian optics so that good understanding of the non-imaging condenser lens is achieved as a good design is derived. As a result, the technique shows the necessity of analytical treatment in contrast to the design approach using only commercial software such as CODE-V, Light-Tools, and others. Of course, CODE V and Light-Tools are also utilized in this paper to confirm and complete the Gaussian optical design.

The Influence of the Stiles - Crawford Effect on the Image (Stiles - Crawford 효과가 결상에 미치는 영향)

  • Park, Seong Jong
    • Journal of Korean Ophthalmic Optics Society
    • /
    • v.5 no.2
    • /
    • pp.175-180
    • /
    • 2000
  • The intensity of beam of light entering near the pupil edge is less than when it passes through the center of the pupil, this phenomenon is known as the Stiles-Crawford effect. In this paper, we investigate the variation in the shape of confusion circle when the real amplitude distribution of incident beam in pupil area is shifted to any direction by effects. The shape of confusion circle on the image surface is rotational symmetric when the real amplitude distribution of incident beam in pupil area isn't shifted, and the shape of confusion circle on the image surface is asymmetric as ellipse when the real amplitude distribution of incident beam in pupil area is shifted. The shifted direction of the real amplitude distribution of incident beam in pupil area equals the major axis direction of confusion circle on the image surface. When the shifted direction of the real amplitude distribution of incident beam in pupil area changes from ${\Delta}{\phi}$ to ${\Delta}{\phi}+{\pi}$, the intensity distributions and the shapes of confusion circle on the image surface for ${\Delta}{\phi}$ equals that for ${\Delta}{\phi}+{\pi}$. We know from above results that the influences of ${\Delta}{\phi}+{\pi}$ and ${\Delta}{\phi}+{\pi}$ cases on the image quality of optical system equal.

  • PDF

Design and Performance of a Catadioptric Omnidirectional Zoom Optical System Using a Hybrid Lens for Visible Light (가시광에서 하이브리드 렌즈를 사용한 반사굴절식 전방위 줌 광학계의 설계 및 성능평가)

  • Park, Hyun Sik;Jo, Jae Heung
    • Korean Journal of Optics and Photonics
    • /
    • v.31 no.2
    • /
    • pp.96-104
    • /
    • 2020
  • A catadioptric omnidirectional zoom optical system using a hybrid lens (COZOSH) that performs simultaneously two functions of a lens and a mirror was designed at the visible wavelength range for daytime unmanned surveillance, and its performance was analyzed. The hybrid lens has lots of advantages in terms of fabrication and assembly of a COZOSH, because of the obviation of a lens boring process and reduction of the number of optical components. Additionally, we designed the COZOSH to expand the compressed inner-image region of a donut image at low spatial frequencies. As a result, the optimized design performance of the optical system that satisfies all initial design specifications was obtained from calculation of the modulation transfer function, spot diagram, and tolerance analysis. We confirmed that the COZOSH is a passively athermalized optical system under conditions of temperature variation from -30℃ to 50℃, by using athermalization analysis during zooming.

A Study of Optical System Design for a Retinal Camera (망막 카메라용 광학계 설계)

  • Hong, Kyung-Hee
    • Korean Journal of Optics and Photonics
    • /
    • v.17 no.2
    • /
    • pp.113-119
    • /
    • 2006
  • We need a good image of the retina of the human eye in order to inspect or cure it. In this work, an optical system design for a retinal camera is studied and the finite schematic eye model made by Sang Gee Kim and Sung Chan Park is used. The optical system is composed of four lens groups. The rays of the entire object field are collected on the center by the 1st group and the objective is imaged by all the other groups. The image is detected by the CCD array and displayed by a monitor The 1st lens group is employed singlet and other groups are employed triplets. Ray aberrations, spot diagrams, diffraction line spread functions and MTFs are calculated for optical performance assessment. This design may be very useful for the development of a retinal camera with high performance.

Tolerance analysis of Multi-Configurative Microscopic System for Inspecting the Wire-Bonding Status of Semiconductor Chips (반도체 와이어 본딩 검사용 다중배치 현미경 광학계에 대한 공차분석)

  • Ryu, Jae-Myung;Kim, Jae-Bum;Kang, Geon-Mo;Jung, Jin-Ho;Baek, Seung-Sun;Jo, Jae-Heung
    • Korean Journal of Optics and Photonics
    • /
    • v.17 no.2
    • /
    • pp.149-158
    • /
    • 2006
  • We have analyzed various tolerances of the multi-configurative microscopic system for inspecting the wire-bonding of a reed frame by using the Gaussian bracket method and the equivalent lens method. The tolerances for the curvature and the thickness, which are axial symmetric tolerances, are given by varying the back focal length within a fecal depth under diffraction-limited conditions. Moreover, by using the trial and error method, the axial non-symmetric tolerances for decenter and tilt are established by assigning the 5% variation of MTF(modulation transfer function) at the spatial frequency of 50 lp/mm and at the field angle of 0.7 field. As the tolerances with the most probable distribution are distributed within the range of the decay rate of less than 5% independent of the probability distribution of tolerances, we can achieve completely the desired design performances of the multi-configurative microscopic system by using the various ranges of these tolerances.

Image quality assessment of color LCD monitors by polychromatic modulation transfer function (다색광전달함수를 사용한 컬러 LCD 모니터의 광학적 상평가법)

  • Song, Jong-Sup;Jo, Jae-Heung;Hong, Sung-Mok;Lee, Yun-Woo;Yang, Ho-Soon;Cho, Hyun-Mo;Lee, In-Won
    • Korean Journal of Optics and Photonics
    • /
    • v.16 no.1
    • /
    • pp.63-70
    • /
    • 2005
  • We propose a method for evaluating the image quality of color liquid crystal display(LCD) monitors by using the polychromatic modulation transfer function(PMTF), which is calculated from the modulation transfer function(MTF) weighted by the overall color response of the system including the test LCD monitor. We confirm that experimental results using the PMTF agree well with simulated results of the PMTF of a color LCD monitor by using three bar targets with different amplitudes and three elementary colors such as red(R), green(G), and blue(B). As a results, we should choose the PMTF instead of the white color MTF or monochromatic MTF in order to evaluate correctly the image quality of color LCD monitors.

The design of microscopic system using zoom structure with a fixed magnification and the independency on the variation of object distance (줌 구조를 이용하여 물체거리가 변해도 상면과 배율이 고정되는 현미경 광학계의 설계)

  • 류재명;조재흥;임천석;정진호;전영세;이강배
    • Korean Journal of Optics and Photonics
    • /
    • v.14 no.6
    • /
    • pp.613-622
    • /
    • 2003
  • The multi-configurative microscopic system for inspecting the wire-bonding of reed frame is designed. Rays refracted by objective lens group which is composed of common lens group of x2 and x6 are splitted by beam-splitter, and Rays through the central region and the boundary region of the object imaged at x2 and x6 through imaging lens groups, respectively. The depth of wire structure on the reed frame has about $\pm$3 mm, in order to observe by uniform magnification without the dependency on the variation of objective distance generated by the depth of wire structure on the reed frame, imaging lens groups should be moved on nonlinear locus like mechanically compensated zoom lenses. The nonlinear equations for zoom locus are derived by using the Gaussian bracket. Refraction powers and positions of each groups are numerically determined by solving the equations, and initial design data for each groups is obtained by using Seidel third order aberration theory. The optimization technique is finally utilized to obtain this microscopic system.