• Journal of the Korean Institute of Telematics and Electronics D
• /
• v.34D no.4
• /
• pp.54-61
• /
• 1997

In this paper, a new holographic display system that can in real-time reconstruct the complex hologram without the bias and the conjugate image, which is obtained form the modified triangular interferometer, is presented. The proposed system is made of adding liquid crystal displays(LCDs), a $\lambda$/2 wave plate, and a polarizing beam splitter to the conventional mach-zehnder interferontric configuration. We demonstrate through theoretical analysis and experiment that real-time image reconstruction from the complex hologram is possible using the proposed system.

• Proceedings of the Korean Society of Machine Tool Engineers Conference
• /
• 2004.10a
• /
• pp.269-273
• /
• 2004

The moduled interferometer with waveplates, polarizing beam splitter, etc. for four phase shifted interference patterns was stabilized with the and Fast Fourier Transform (FFT) method was used to investigate the surface profile measurement from the interferenece pattern from Twyman-Green interferometer using a mathcad.

• Proceedings of the Optical Society of Korea Conference
• /
• 2003.02a
• /
• pp.266-267
• /
• 2003

Home Theater를 비롯한 대화면 디스플레이에 주로 사용되는 전면 투사방식의 프로젝션은 현재 소형화와 경량화를 위한 연구가 진행되고 있다. 프로젝션 디스플레이 장치는 기본적으로 조명 광학계와 투사 광학계로 구성되어지는데, 소형화와 경량화를 위해서는 광학 부품의 수를 줄이고 각 부품의 설계 및 구성, 배치를 최적화 시켜야 하고 이를 위하여 조명 광학계의 구성을 최적화하는 것이 필수적이다. 일반적인 프로젝션 조명 광학계 구성은 Beam splitter, 전반사 프리즘, Mirror 방식 등을 적용하고 있다. (중략)

• Bulletin of the Korean Space Science Society
• /
• 2009.10a
• /
• pp.25.1-25.1
• /
• 2009

적외선 우주배경복사 관측실험 (Cosmic Infrared Background ExpeRiment, CIBER) II는 2009년 2월 25일 화이트샌드 미사일 기지에서 NASA 사운딩 로켓에 탑재, 발사된 CIBER I의 후속 프로젝트이다. 독립적인 Imager 2 대와 Spectrometer 2 대로 구성된 CIBER I과 달리 CIBER II는 하나의 주경과 부경으로 구성된 광학계를 4 대의 Imager가 beam splitter를 이용하여 관측하게 구성되어 있다. CIBER II는 NASA에서 공식적으로 승인되었으며, 한국천문연구원과 한국기초과학지원연구원이 미국 NASA/JPL, Caltech 및 일본 ISAS와 국제 공동으로 개발할 계획이다.

• Proceedings of the Optical Society of Korea Conference
• /
• 2003.07a
• /
• pp.228-229
• /
• 2003

광자 크리스탈의 밴드 구조가 다른 물질이 접하는 경계면으로 구성되는 이종 접합 구조(Heteorostructure)는 단일 구조에서 관찰할 수 없는 특성을 보유하고 있으므로 관심을 끌고 있다. 이를 이용한 다 파장 add-drop 필터, 2D-3D 하이브리드 구조에 의한 무 회절 손실 도파로, beam splitter와 combiner 등의 연구 결과가 최근에 제시되었다. 본 논문에서는 positive 굴절율과 negative 굴절율을 갖는 광자 크리스탈이 이종 접합 구조를 형성할 때의 굴절 작용의 변화를 실린더의 반지름 변화에 따라 고찰하였다. (중략)

• Proceedings of the Optical Society of Korea Conference
• /
• 2003.07a
• /
• pp.18-19
• /
• 2003

측면 연마 광섬유 결합기는 비록 제작 공정이 다소 복잡하지만 다양한 응용이 가능하기 때문에 많은 연구가 진행 되어 왔다. 특히 최근에는 광센서나 초고속 광통신망에 편광 유지 광섬유를 이용한 광학소자의 필요성이 증가 하고 있다. 본 논문은 얇은 중간 금속 층을 가지는 측면 연마 편광 유지 광섬유 결합기를 이용한 편광 분리기에 관한 실험 연구 결과를 보고한다. (중략)

• Journal of the Korea Institute of Information and Communication Engineering
• /
• v.9 no.1
• /
• pp.160-164
• /
• 2005

The process of recognizing a vehicle involves detection of the vehicle, recognition of the vehicle model, and identification of the vehicle. The process of vehicle identification involves identification of the vehicle itself, such as by recognition of the license plate on the vehicle. In this paper the method involves the use of a beam splitter to divide incident rays into two directions, a transmitted beam and a reflected beam of different light intensities, and synthesizing two captured images using CCD devices from each beam, thus producing fluctuation-free images of a wide dynamic range even when the subject is moving. A prototype license plate recognition system was also developed using the experimental sensing device. The system achieved a 98.7% recognition rate on 466 images of moving vehicles, which demonstrates its effectiveness as a license plate recognition system.

• Korean Journal of Optics and Photonics
• /
• v.14 no.6
• /
• pp.657-662
• /
• 2003

Optimum Hamming apodized acousto-optic 2${\times}$2 add/drop multiplexers, using SiO$_2$ film loaded acoustic waveguide with angular offset to the Ti:LiNbO$_3$ waveguide, were fabricated. The four-port device consists of two input waveguides, a polarization beam splitter (PBS), two polarization conversion/acoustooptic tuning waveguide sections, a second PBS and two output waveguides. Insertion loss <7.1 ㏈ has been obtained and side-lobe of -19 ㏈ for -32 ㎽ RF driving power has been realized. Add/drop performance has been confirmed and a linear tuning rate of 8.1 nm/MHz and a 3 ㏈ spectral width of -1.5 nm were demonstrated.

• Korean Journal of Optics and Photonics
• /
• v.23 no.6
• /
• pp.274-280
• /
• 2012

A normal incidence ellipsometer is fabricated to measure the optical anisotropy of a small spot whose diameter is less than $8.0{\mu}m$, by adding a beam splitter and a prism to the conventional rotating analyzer type ellipsometer. The polarizing actions of the added optical components are calibrated to improve the accuracy of the anisotropy measurement. The standard deviation of the optical anisotropy factor decreased to 0.00083, and the variation of the optical anisotropy factor of rutile versus sample azimuth angle variation also decreased to 0.015, after adoption of a non-polarizing beam splitter and a quarter wavelength phase retarder, followed by removal of the optical fiber and a careful choice of measurement wavelength.

• Korean Journal of Optics and Photonics
• /
• v.9 no.6
• /
• pp.368-372
• /
• 1998

A 16-views 3 dimensional imaging system is designed by spatially combinding two 8-views time multiplexed image channels. Each 8-views channel composed of 3 primary color CRTs and a dichroic beam splitter which combining the three CRTs as one channel. Each CRT displays 8-view images time sequentially. These images are projected to a holographic screen of a size 1$\times$0.8 $m^2$ through a projection optics. Characteristics of the three different configurations of projection optics are examined with the optics designing program "DEMOS" to select an optimized projection optics for the system. The configulation of the optimized projection optics is found like following; images from each channel combined by two-fold mirror are projected by a projection objective through a 16-strips LCD shutter. In this configuration, the shutter should be located at the entrance pupil of the objective, and the folded edge of the two-fold mirror should contact symmetrically to the center line of the shutter.e shutter.