• Title/Summary/Keyword: Lens array

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Orthoscopic integral imaging by use of concave-convex lens array coupling (오목-볼록 렌즈 어레이 결합을 이용한 orthoscopic 집적결상)

  • 서장일;차성도;신승호
    • Proceedings of the Optical Society of Korea Conference
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    • 2003.02a
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    • pp.238-239
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    • 2003
  • 집적결상(integral imaging)에서 렌즈어레이(lens array)를 이용하여 3차원적인 물체를 기본영상(elemental image)들로 결상한 후, 다시 그 기본 이미지들로부터 3차원 이미지를 재생하는 과정에서 기본 이미지들을 변환시키지 않으면, 3차원 이미지가 재생될 때, 렌즈어레이와 수직한 축에 대해 렌즈어레이에 가까운 쪽과 먼 쪽이 서로 바뀌는 슈도스코픽(pseudoscopic) 현상이 일어난다. 그래서 기본이미지들을 변환시키기 위해 렌즈어레이를 한번 더 사용한 이단 집적결상계를 이용하거나 영상처리 방법을 이용하는데, 이와 같은 방법은 광학적 손실을 크게 하거나 처리 속도를 느리게 한다. (중략)

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Fabrication of micro-lens arrays using a grayscale mask (그레이스케일 마스크를 이용한 미소렌즈 배열의 제작)

  • 조두진;성승훈
    • Korean Journal of Optics and Photonics
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    • v.13 no.2
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    • pp.117-122
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    • 2002
  • Some 10$\times$10 micro-lens arrays of a period of 300 ${\mu}{\textrm}{m}$, a thickness of 17 ${\mu}{\textrm}{m}$, and a focal length of 2.2 mm are fabricated by exposing a thick layer of photoresist through a grayscale mask via UV proximity printing. The grayscale mask is fabricated in a holographic film by reducing (6.6X) a high-resolution black-and-white film where a grayscale patters of a micro-lens array designed by a computer has been written using a film recorder. The proposed method has the advantage of a low fabrication cost, a fill-factor of almost 100% and the ease of realizing an aspheric lens.

Optical Analysis for the Autostereoscopic Display with a Lenticular Array Using Finite Ray Tracing (유한광선추적을 이용한 렌티큘러 렌즈 기반 3차원 디스플레이 장치의 해석)

  • Kim, Bong-Sik;Kim, Keon-Woo;Choi, Da-Shin;Park, Woo-Sang
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.27 no.3
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    • pp.162-166
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    • 2014
  • We propose an analysis method of an autostereoscopic display system with lenticular lens array using finite ray-tracing method that is verified by the geometrical optics. In the present work, we adopt the cylinder equation for the mathematical expression of the lenticular lens. For the calculation of the direction cosine of the transmitted ray, we first calculate the refracting point at bottom of the lens and the direction cosine of the incident ray that propagating through the lens by the Snell's law, and then apply to finite ray-tracing method. Finally, we obtain the simulation results for the intensity distribution of the ray at optimal viewing distance. From these results, we confirm the realization of 3D image that exists separately according to the viewing position at an optimal viewing distance.

Numerical Reconstruction of Two-dimensional Object from the Image Captured by a Random Lens Array (불규칙 렌즈 배열을 통과한 영상을 이용한 2차원 물체의 수치적 복원)

  • Hong, Sung-In;Kim, Nam;Park, Jae-Hyeung
    • Korean Journal of Optics and Photonics
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    • v.24 no.3
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    • pp.120-124
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    • 2013
  • We propose a method to reconstruct the two-dimensional object from an image captured through an array of random lenses each of which has random shape, size, and focal power. In the proposed method, the characteristics of the random lens array are estimated by capturing images for known elementary inputs, and then the object is reconstructed by measuring correlations between the random lens images of the object and the elementary inputs. The experimental results show that the original object can be recognized by the proposed reconstruction method. Nevertheless, further quality enhancement is required to increase feasibility and to extend to general three-dimensional object cases.

Fabrication of Silicon Nanotemplate for Polymer Nanolens Array

  • Cho, Si-Hyeong;Kim, Hyuk-Min;Lee, Jung-Hwan;Venkatesh, R. Prasanna;Rizwan, Muhammad;Park, Jin-Goo
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2011.05a
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    • pp.37.1-37.1
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    • 2011
  • Miniaturization of lenses has been widely researched by various scientific and engineering techniques. As a result, micro scaled lens structure could be easily achieved from various fabrication techniques; nevertheless it is still challenging to make nano scaled lenses. This paper reports a novel fabrication method of silicon nanotemplate for nanolens array. The inverse structure of nanolens array was fabricated on silicon substrate by reactive ion etching (RIE) process. This technique has a flexibility to produce different tip shapes using different pattern masks. Once the silicon nano-tip array structure is well-defined using an optimized recipe, it is followed by polymer molding to duplicate nanolens array from the template. Finally, the nanostructures formed on silicon nanotemplate and polymer replica were investigated using FE-SEM and AFM measurements. The nano scaled lens can be manufactured from the same template, also using other replication techniques such as imprinting, injection molding and so on.

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A New Shack-Hartmann Type Wavefront Sensor Using Liquid Crystal Panels

  • Xiaoxi, Chen;Xu, Liu
    • 한국정보디스플레이학회:학술대회논문집
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    • 2005.07a
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    • pp.528-530
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    • 2005
  • In this paper, we present a new and practical method for achieving real-time wavefront measurement, dramatically increasing the resolution, dynamic range of Shack-Hartmann wavefront sensor and improving the wavefront reconstruction quality. In proposal method, a liquid crystal display panel (LCD) for the generation of an array of Fresnel microlenses is use instead of the static microlens array of the conventional Shack-Hartmann type sensor. An off-axis holographic microlens array is designed instead of the normal microlens array to increase the effective array and then the dynamic range. The focus properties of the off-axis lens are studied.

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An effective parallel optical interconnection using single GRIN rod lens (하나의 GRIN Rod Lens를 이용한 효율적 병렬 광연결)

  • Kim, Sung-Chul;Lee, Wook;Lee, Byoung-Ho;Jeong, Ji-Chai
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.34D no.1
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    • pp.49-54
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    • 1997
  • We proved the feasibiltiy of a parallel optical interconnection technique using single GRIN (graded-index) rod lens as an intermediate coupling device, which increases the working distance and makes packaging easy. The proposed technique shows relatively less dependency on misalignments. In this paper, for convensience of experiments, we applied this method to 4-channel coupling between two fiber arrays, and compared it with butt-coupling and the method of using ball lens. The comparison shows the feasibility of adopting the proposed method to the parallel interconnection between a laser diode array and an optical fiber array.

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A Theoretical Design of RADANT Lens (RADANT 렌즈의 이론적 설계에 관한 연구)

  • Lee, Kee-Oh;Park, Dong-Chul
    • Journal of the Korea Institute of Military Science and Technology
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    • v.12 no.3
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    • pp.360-367
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    • 2009
  • In this paper, the RADANT phase scanning scheme and the transmission-type loaded line phase shifter scheme, which are applicable to the phased array systems, are studied. Using these two schemes, a theoretical method to design an electronic beam steering RADANT lens is introduced. The validity of the presented theoretical method is verified through the simplified circuit simulation results.

Fabrication of refractive PMMA microlens array using transparent acrylic resin (투명 아크릴 레진을 이용한 초소형 PMMA 렌즈 배열의 제작)

  • Ahn, Si-Hong;Kim, Yong-Kweon
    • Proceedings of the KIEE Conference
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    • 1999.07g
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    • pp.3316-3318
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    • 1999
  • PMMA(poly-methyl methacrylate) microlens array is fabricated using transparent acrylic resin. PMMA is commonly used material for plastic lens due to its excellent visibility larger than 90% and other optical characteristics so much close to those of glass. Orthodontic resin (DENTSPLY International Inc.), commonly used in dentistry, is an transparent acrylic resin kit including MMA liquid and polymerization powder. Their mixture results in PMMA through polymerization. Using the resin PMMA layer is formed on the substrate through spin-coating. Designed pattern of lens structure is transferred to PMMA layer by RIE (Reactive Ion Etching) with oxygen plasma. Final lens shape is formed by thermal treatment that causes PMMA to reflow, The thickness of PMMA spun on the substrate is $17{\mu}m$ that is also final sag of microlens, Designed diameters of the microlenses are $200{\mu}m$, $300{\mu}m$,and $500{\mu}m$, respectively.

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