• 한국안광학회지
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• 제5권1호
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• pp.1-6
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• 2000

본 연구는 안경렌즈와 안광학계를 광학계로 이루고 있는 합성광학계에 wavelength는 3가지로 ${\omega}{\upsilon}_1=0.588{\mu}$, ${\omega}{\upsilon}_2=0.486{\mu}$ ${\omega}{\upsilon}_3=0.656{\mu}$로 하였고 Entrance Beam Radius(mm)는 1mm로 Field angle(deg)는 5.7296e-0.5, Image Aperture는 0.053055 mm, Exit Aperture는 0.903711 mm로 Reflective focal length는 25.181514 mm, Petzval radius는 -19.21839 mm, n=1.523의 조건에서 OSLO를 이용하여 spot size, focus shift, optical focus를 산출하였다. spot size는 후면곡률반경이 1 mm~30 mm까지는 0.002 mm~0.07 mm size가 다음과 같이 큰 수치로 나타났고 50 mm 이상에서는 거의 비슷한 0.0005 mm~0.002 mm가 나왔고 focus shift에서는 3가지 종류의 렌즈에서 50 mm가 focus shift가 적게 나타났고 전체적인 경향은 1 mm~15 mm 까지는 수치가 높다가 25 mm까지는 낮아지다가 다시 높아지는 양상을 보였으며 optical focus는 100 mm가 가장 좋았고 100 mm 렌즈를 후면곡률반경으로 하여 optical focus 산출하였으며 산출한 optical focus를 최적화한 결과 값이 $60{\pm}1mm$로 나타났다.

• Journal of the Optical Society of Korea
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• 제1권2호
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• pp.74-80
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• 1997

300mm F/4.0 telephotolens with diffractive hybrid lens was designed, and its optical performance was tested and compared with a traditional lens system. DOE(Diffractive Optical Element) reconstructs wavefronts using wave phenomena of light to focus the incident light onto the focal point and has negative Abbe number while a traditional lens uses geometrical phenomena of light and has positive Abbe number. Therefore, a diffractive hybrid lens containing both refractive and diffractive elements can remarkably correct chromatic aberration and spherical aberration of an optical system. We investigated and analyzed the optical properties of a diffractive hybrid lens for the visible spectrum, and we used a difractive hybrid lens to design and evaluate a 300mm F/4.0 telephotolens without the special LD(Low Dispersive) glass lens which is costly and difficult to manufacture. Most traditional telephotolenses use the special LD glass for chromatic aberration correcton. Optical performance tests such as resolution and characteristics of aberration of both lens systems using a diffractive hybrid lens and traditional lens were performed.

• 한국기계가공학회지
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• 제19권6호
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• pp.96-101
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• 2020

In this paper, we present the results of our research to perform 3D laser scanning functions by adding a focusing lens to a conventional 2D laser scanner. For the optical design, the ray-tracing technique was used along with a total of four lenses as the variable incident focusing lens, the collimating lens, and the F-Theta lens. As design variables, the curvature of the incident focusing lens (Lens #1) was assumed to be us, l mm and sumed mm, and the incident angles were set at 0cidenus, l. In addition, the distance between the focusing lens and the collimating lens was set to vary from 5 mm to 15 mm. When the incident focal length was varied from 5 mm to 15 mm, the exit focal length was calculated to vary from 67.5 mm to 56.8 mm for the lens with R = 100 mm and from 108.5 mm to 99.0 mm for the lens with R = 150 mm. When the incident angle was 0°, the focal aberration was only slightly observable at 10㎛ in both the x- and y-direction. At 7.5° was the focal aberration of approximately 20~50㎛ was measured at 20㎛. To investigate the chromatic aberration of the designed optical device, the distortion of the focus was observed when the 550 nm beam was simulated on lens designed for a 980 nm wavelength.

• Journal of the Optical Society of Korea
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• 제18권2호
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• pp.134-145
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• 2014

The number of lens groups in modern zoom camera systems is increased above that of conventional systems in order to improve the speed of the auto focus with the high quality image. As a result, it is difficult to calculate zoom loci using the conventional analytic method, and even the recent one-step advanced numerical calculation method is not optimal because of the time-consuming problem generated by the iteration method. In this paper, in order to solve this problem, we suggest a new unified analytic method for zoom lens loci with finite object distance including infinite object distance. This method is induced by systematically analyzing various distances between the object and other groups including the first lens group, for various situations corresponding to zooming equations of the finite lens systems after using a spline interpolation for each lens group. And we confirm the justification of the new method by using various zoom lens examples. By using this method, we can easily and quickly obtain the zoom lens loci not only without any calculation process of iteration but also without any limit on the group number and the object distance in every zoom lens system.

• 한국정밀공학회지
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• 제33권6호
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• pp.459-467
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• 2016

Using a line scan camera and a Galvano mirror, we constructed a high-speed line-scanning microscope that can generate 2D images ($8000{\times}8000pixels$) without any moving parts. The line scanner consists of a Galvano mirror and a cylindrical lens, which creates a line focus that sweeps over the sample. The measured resolutions in the x (perpendicular to line focus) and y (parallel to line focus) directions are both $2{\mu}m$, with a 2X scan lens and a 3X relay lens. This optical system is useful for measuring defects, such as spalling, chipping, delamination, etc., on the surface of carbon fiber reinforced plastic (CFRP) holes after machining in conjunction with adjustments in the angle of LED lighting. Defects on the inner wall of holes are measured by line confocal laser scanning. This confocal method will be useful for analyzing defects after CFRP machining and for fast 3D image reconstruction.

• 전자공학회논문지B
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• 제29B권2호
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• pp.40-49
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• 1992

In this paper,a new approach-using the linear movement of the lens location in a camera and focal distance in each location for the measurement of the depth of the 3-D object from several 2-D images-is proposed. The sharply focused edges are extracted from the images obtained by moving the lens of the camera, that is, the distance between the lens and the image plane, in the range allowed by the camera lens system. Then the depthin formation of the edges are obtained by the lens location. In our method, the accurate and complicated control system of the camera and a special algorithm for tracing the accurate focus point are not necessary, and the method has some advantage that the depth of all objects in a scene are measured by only the linear movement of the lens location of the camera. The accuracy of the extracted depth information is approximately 5% of object distances between 1 and 2m. We can see the possibility of application of the method in the depth measurement of the 3-D objects.

• 한국레이저가공학회지
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• 제12권2호
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• pp.26-30
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• 2009

Scanning Electron Microscopy (SEM) includes high voltage generator, electron gun, column, secondary electron detector, scan coil system and image grabber. Column includes electron lenses (condenser lens and objective lens). Condenser lens generates fringe field, makes focal length and control spot size. Focal length represents property of lens. Objective lens control focus. Most of the electrons emitted from the filament, are captured by the anode. The portion of the electron current that leaves the gun through the hole in the anode is called the beam current. Electron beam probe is called the focused beam on the specimen. Because of the lens and aperture, the probe current becomes smaller than the beam current. It generate various signals(backscattered electron, secondary electron) in an interaction with the specimen atoms. In this paper, we describe the result of research to develop the core elements for low-resolution SEM.

• 한국측량학회지
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• 제26권1호
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• pp.93-100
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• 2008

줌 렌즈를 이용해 피사체를 촬영할 때 카메라 렌즈의 줌, 포커스, 조리개수치와 같은 요소들은 촬영 현장의 상황에 따라 변하게 된다. 특히 줌 조작을 하여 카메라 렌즈의 초점거리를 변화시키면 렌즈의 기하학적 배열은 크게 변하기 때문에 렌즈모델도 그에 따라 변하게 된다. 본 연구에서는 일반적인 카메라의 촬영 조건하에서 줌 조작시 렌즈모델이 어떻게 변하는지를 조사하였다. 이를 위해 포커스와 조리개 등의 요소를 카메라가 임의로 조절하는 상황에서도 모델의 각 요소들을 효과적으로 모델링할 수 있는지를 검토해보았다. 이를 위해 렌즈모델 추정을 위한 이미지를 촬영후 각각의 초점거리별로 자체검정을 실시하여 렌즈모델의 각 변수들을 수집하고 정리하였다. 그리고 수집된 데이터에서 패턴을 찾아 매개변수의 변화 양상이 특정한 패턴을 보이는지 관찰하였다. 그 결과 포커스와 조리개 수치를 통제하지 않는 조건임에도 불구하고 방사왜곡과 관련된 매개변수에서 일정한 패턴이 관찰되었으며 특히 방사왜곡의 2차항의 계수가 뚜렷한 선형성을 가지고 있음이 확인되었다. 이 계수를 모델링하고 촬영시의 초점거리를 알고 있으면 영상 촬영시 줌 조작을 하여도 별도의 자체검정 과정 없이 영상의 왜곡을 상당부분 제거할 수 있을 것으로 기대된다.

• Journal of the Optical Society of Korea
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• 제20권3호
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• pp.407-412
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• 2016

We analyzed through numerical simulations the properties of a square beam homogenizer near the target for laser shock peening. The efficiency was calculated near the target by considering the plasma threshold of the metals. We defined the depth of focus of the square beam homogenizer with a given efficiency near the target. Then, we found the relationship between the depth of focus for the laser shock peening and four main parameters of the square beam homogenizer: the plasma threshold of the metal, the number of lenslets in the array-lens, the focal length of the condenser lens and the input beam size.

• 한국정밀공학회지
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• 제21권3호
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• pp.74-82
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• 2004

This paper proposes a fast zooming and focusing technique for implementing a real-time surveillance camera system which can capture a face image in less than 1 second. It determines the positions of zooming and focusing lenses using two-step algorithm. In the first step, it moves the zooming and focusing lenses simultaneously to the positions calculated using the lens equations for achieving the predetermined magnification. In the second step the focusing lens is adjusted so that it is positioned at the place where the focus measure is the maximum. The camera system implemented for the experiments has shown that the proposed algorithm spends about 0.56 second on average fur obtaining a focused image.