• 한국광학회지
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• 제34권3호
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• pp.117-123
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• 2023

반사경의 광학면이 넓어질수록 높은 공간 주파수 형상이 광학계의 성능에 큰 영향을 주므로, 대형 반사경 성능 평가에서 이를 측정할 수 있어야 한다. 따라서 높은 주파수의 형상을 샘플링할 수 있는 고해상도 형상 측정 시스템이 필요하다. 본 연구에서는 반사경의 고해상도 형상 측정을 위한 회전 프리즘 정합 간섭계(rotational prism stitching interferometer, RPSI)라는 새로운 방법을 제안한다. RPSI는 기존에 사용되고 있는 상용 간섭계에 빔 확장 렌즈, 이송 거울, 회전 프리즘 등을 추가하여 구성되었으며, 간섭계를 움직이지 않고 원통 좌표계를 기준으로 전체 구경을 아우르는 부분 구경 형상들을 측정한다. 측정된 부분 구경들은 최소자승법을 이용한 부분 구경 정합법을 이용하여 정합되며, 빔확장 렌즈 배율의 제곱만큼 높은 샘플링 밀도로 전체 구경 형상 정보를 복원 가능하다. 3배율을 가지는 RPSI를 이용하여 직경 40 mm의 구면 반사경 형상을 측정하였고, 간섭계 단독으로 측정한 전체 구경 형상과 비교 검증하였다. 약 1 nm RMS의 근소한 차이로 유사한 형상을 잘 복원할 수 있었으며, 간섭계 단독으로 사용한 형상 측정 결과보다 렌즈의 배율의 제곱배만큼 향상된 샘플링 밀도로 형상 측정이 가능함을 확인하였다.

• Journal of the Optical Society of Korea
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• 제19권1호
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• pp.55-62
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• 2015

In this study we demonstrate ultrahigh-resolution spectral domain optical coherence tomography (UHR SD-OCT) with a linear-wavenumber (k) spectrometer, to accelerate signal processing and to display two-dimensional (2-D) images in real time. First, we performed a numerical simulation to find the optimal parameters for the linear-k spectrometer to achieve ultrahigh axial resolution, such as the number of grooves in a grating, the material for a dispersive prism, and the rotational angle between the grating and the dispersive prism. We found that a grating with 1200 grooves and an F2 equilateral prism at a rotational angle of $26.07^{\circ}$, in combination with a lens of focal length 85.1 mm, are suitable for UHR SD-OCT with the imaging depth range (limited by spectrometer resolution) set at 2.0 mm. As guided by the simulation results, we constructed the linear-k spectrometer needed to implement a UHR SD-OCT. The actual imaging depth range was measured to be approximately 2.1 mm, and axial resolution of $3.8{\mu}m$ in air was achieved, corresponding to $2.8{\mu}m$ in tissue (n = 1.35). The sensitivity was -91 dB with -10 dB roll-off at 1.5 mm depth. We demonstrated a 128.2 fps acquisition rate for OCT images with 800 lines/frame, by taking advantage of NVIDIA's compute unified device architecture (CUDA) technology, which allowed for real-time signal processing compatible with the speed of the spectrometer's data acquisition.

• 대한기계학회논문집
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• 제17권9호
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• pp.2286-2293
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• 1993

The study presents the development of a cost-effective CAD/CAM system for metal moulds by use of personal computer. In the personal CAD/CAM system named DKSYS, metal moulds are defined by the operations of basic elements such as prism, pyramid and sphere, plane, rotational body, and surface elements including curved surface. The internal expression of shape elements in the computer is based on the wire model, which is a set of cross-sectional curves of the shape elements. With the addition of OMS system to CAD/CAM system the optimum cutting condition can be selected automatically. After programming NC information with the form definition and the optimum cutting condition, the metallic mould can be formed by transferring cutting information to CNC machine through DNC system. Using a computer for the above process, it is possible to increase the productivity and reduce the cost.

• Tribology and Lubricants
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• 제32권2호
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• pp.50-55
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• 2016

Recently, a double-side machining process has been adopted in fabricating a sapphire glass to enhance the manufacturability. Double-side lap grinding (DLG) is one of the emerging processes that can reduce process steps in the fabrication of sapphire glasses. The DLG process uses two-body abrasion with fixed abrasives including pallet. This process is designed to have a low pressure and high rotational speed in order to obtain the required material removal rate. Thus, the temperature is distributed on the DLG platen during the process. This distribution affects the shape of the substrate after the DLG process. The coolant that is supplied into the cooling channel carved in the base platen can help to control the temperature distribution of the DLG platen. This paper presents the results of computational fluid dynamics with regard to the heat transfer in a DLG platen, which can be used for fabricating a sapphire glass. The simulation conditions were 200 rpm of rotational speed, 50℃ of frictional temperature on the pallet, and 20℃ of coolant temperature. The five cases of the coolant flow rate (20~36 l/min) were simulated with a tetrahedral mesh and prism mesh. The simulation results show that the capacity of the generated cooling system can be used for newly developed DLG machines. Moreover, the simulation results may provide a process parameter influencing the uniformity of the sapphire glass in the DLG process.

• 한국광학회지
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• 제12권1호
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• pp.25-31
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• 2001

1차원 이동 변위를 격자의 피치 p보다 1/10 이하의 작은 정밀도로 측정이 가능한 elongated circular gratign(EC 격자)를 가간섭 광원으로 조명하여 Talbot 거리에서 일어나는 Talbot 효과를 실험적으로 확인하였다. 그리고 서로 다른 주기를 갖는 렌즈없이 결상된 EC 격자의 Talbot 상과 고정된 EC 격자의 상호 변위시 이들의 중첩에 의한 Talbot 무아레 무늬를 만들었으며 이를 이용한 한 예로 경사진 평행판의 경사각 정도를 측정하였다. 그리고 한 EC 격자의 Talbot 상과 그 자체의 EC 격자와의 무아레 현상을 이용하여 거울정렬시 미세한 회전각을 가시적으로 매우 쉽게 측정하는 방법을 제안하고 실험하였다.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2005년도 춘계학술대회 논문집
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• pp.1223-1227
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• 2005

Fine microgroove is the key component to fabricate micro-grating, micro-grating lens and so on. Conventional groove fabrication methods such as etching and lithography have some problems in efficiency and surface integrity. This study deals with the creation of ultra-precision micro grooves using non-rotational diamond tool and CNC machining center. The shaping type machining method proposed in the study allows to produce V-shaped grooves of $40\mu{m}$ in depth with enough dimensional accuracy and surface. For the analysis of machining characteristics in micro V-grooving, three components of cutting forces and AE signal are measured and processed. Experimental results showed that large amplitude of cutting forces and AE appeared at the beginning of every cutting path, and cutting forces had a linear relation with the cross-sectional area of uncut chip thickness. From the results of this study, proposed micro V-grooving technique could be successfully applied to forming the precise optical parts like prism patterns on light guide panel of TFT-LCD.