• Current Optics and Photonics
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• 제8권3호
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• pp.307-312
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• 2024

Measuring the three-dimensional (3D) spatial light intensity distribution of an autostereoscopic multiview 3D display at the user position is time-consuming, as luminance has to be measured at different positions around the user position. This study investigates a method to quickly estimate the 3D distribution at the user position. For this purpose, a measurement setup using a white semitransparent diffusing screen or a two-dimensional (2D) spatial sensor was devised to measure the 2D light intensity distribution at the user position. Furthermore, the 3D spatial light intensity distribution at the user position was estimated from these 2D distributions at different viewing distances. From the estimated 3D distribution, the characteristics of autostereoscopic 3D display performance can be derived and the candidate positions for further accurate measurement can be quickly determined.

• 한국레이저가공학회지
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• 제15권2호
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• pp.11-14
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• 2012

In this paper, we have made a proposal concerning the beam shaping mask(BSM) using random-array slits to control intensity distribution profile of laser beam and demonstrated its proprieties experimentally. When a lot of slits are set out irregularly, diffraction patterns of light does not appear but granularity patterns as a bundle of fibers appear. Intensity distribution profile is controlled by densities distribution of circular slits arrayed randomly because the number of slits and its area means amount of light energy through BSM. Namely as the number of slits in high intensity area is increased and that in low intensity area decreased, amount of light energy is same over all local parts. So gaussian intensity distribution could be changed to flat-top.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2000년도 추계학술대회 논문집
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• pp.43-46
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• 2000

Optical triangulation displacement sensors(0TDSs) are widely used for their simple struchlre, high resolution, and long operating range. However, there are several factors that must be taken into account in order to obtain high accuracy and reliability Measurement errors from inclinations a？ an object surface, prohe signal fluctuations generated by speckle effects. power vanation of a light source, electronic noises, and so on. Previous models of OTDSs can not show reasonable behavior as change of surface inclination and shape of light intensity distribution on the detector. In this paper, we propose a new and reasonable modeling for diffise-type OTDSs based on a geometrical optics. To verify propriety of new modeling, we take basic experiments. Shape of light intensity distribution is asymmetric in both simulation result and experimental result. Both simulation result and experimental result show same tendency of light intensity distribution movement as changing surface inclination

• The Korean Journal of Ecology
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• 제20권4호
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• pp.285-291
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• 1997

The taxonomic characteristics of Eupatorium rugosum were reviewed and growth responses under different light intensities were investigated. Changes of soil and vegetation environments at experimental plots on Mt. Namsan were surveyed and the distribution pattern examined. The distribution of E. rugosum was closely related to the content of total nitrogen and available phosphorus in the soil. No competitors which could inhibit the growth of E. rugosum were present. Growth of E. rugosum was highest at a light intensity of 7, 500 lux, but dry weight was highest at a light intensity of 15, 000 lux followed by 30, 000 and 7, 500 lux. Growth in height of E. rugosum under a light intensity of 1, 500 lux continued even though the amount of growth was small. E. rugosum is found throughout the area of Mt. Namsan, and its density is higher at the roadside and in valley regions. E. rugosum appeared at 25 of 50 quadrats on Mt. Namsan, and the mean coverage of E. rugosum in survey quadrats was 12%.

• 정보저장시스템학회논문집
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• 제6권1호
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• pp.1-5
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• 2010

Holographic data storage system(HDSS) has many noise sources - crosstalk, scattering and inter pixel interference, etc. Generally the intensity of a light generated from the laser source has Gaussian distribution and this ununiformity of light also can make the data page to have a low SNR. A beam apodizer is used to make the laser as a flat-top beam but the intensity distribution is not strictly uniform. The intensity of light can be controlled using image mask. In this paper the intensity distribution of light used for HDSS is controlled by a digital image mask. The digital image mask is changed arbitrarily in real-time with suggested algorithm for the HDSS.

• 한국조명전기설비학회:학술대회논문집
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• 한국조명전기설비학회 2005년도 춘계학술대회논문집
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• pp.14-18
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• 2005

It is important to select light sources and luminaires in the process of lighting design. Therefore, development of light sources has been constantly grown for a high efficacy and long life. And, the design of luminaires has been developed for the reflection of light mechanism. But it has been not enough to study for the refraction of light mechanism Therefore, the propose of this study is to study for the refraction of light mechanism. In addition, this study is modeling for the luminous intensity distribution of planar prism to use the results of photometric data that is able to obtain various luminous intensity distribution.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2002년도 춘계학술대회 논문집
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• pp.263-266
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• 2002

An optical method for surface roughness estimation based on statistical analysis of the light intensity of a scattered laser beam pattern. The method is very simple but has a disadvantage that no more information than the averaged roughness is estimated. In this study a new try was conducted to derive more advanced surface information from the details of the light intensity distribution. Some periodic ripples among the light intensity distribution being assumed to relate with scratch left on the machined surface, a corresponding surface profile is estimated from the ripples using FFT and IFFT algorithm. IFFT technique is used to extract some dominant signal components among the intensity distribution. Compared to the measured profiles by a stylus type surf-tester, the profiles obtained through the proposed method are probably acceptable in a sense of the profile shape. Calibration of the amplitude needs more works in the future.

• 한국통신학회논문지
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• 제37권8A호
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• pp.698-705
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• 2012

무안경 방식 스테레오스코픽 입체 디스플레이 시스템에서 시역간 크로스토크는 입체시를 저해하는 주요 문제이다. 기존 크로스토크에 대한 연구는 관찰자면에서 수평 방향으로 인접한 시역간 겹침비를 정량적으로 분석하는 것이 대부분이었으나, 본 연구에서는 이를 포함, 깊이 방향으로 형성되는 해당시점영상의 밝기분포를 정량화하여 수평, 깊이방향에 따른 유효 관찰영역을 제시함으로서 효과적인 입체시 시청 범위를 제공하는데 목적을 두었다. 본 논문에서는 무안경방식의 스테레오스코픽 입체 디스플레이 환경에서 유발되는 크로스토크의 주요 인자들을 디스플레이 환경 및 관찰환경에서 도출하고 이들의 관계를 정성적으로 분석할 수 있는 알고리듬 개발 및 이를 가시화 할 수 있는 시뮬레이션 툴을 제작하였다. 더불어 시뮬레이션 결과를 응용하여 관찰자를 최적의 입체시 시청영역으로 유도 할 수 있는 최적입체시 가이드 시스템을 제안하였다.

• 한국광학회지
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• 제12권2호
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• pp.103-108
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• 2001

플라즈마 디스플레이 패널(plasma display panel :PDP)에서 방출되는 광의 3차원 분포를 측정하기 위한 scanned point-detecting system(SPDS)을 고안하여 제작하였으며 이 시스템을 이용하여 실제 PDP의 3차원 광 방출 특성을 측정하고 해석하였다. SPDS는 상면에 핀홀이 달려 있는 광검출기(point detector)를 위치시킴으로써 특정 지점으로부터 방출되는 광만을 검출할수 있다. 3차원 물체의 특정 지점으로부터 방출된 광은 핀홀을 지나 검출기로 모두 입사되지만 다른 지점으로부터 방출된 광은 핀홀 앞에서 미리 집속되거나 핀홀 뒤에서 집속될것이므로 이러한 광들은 핀홀에 의해 대부분 차단될 것이다. 그러므로 물체의 특정 지점으로부터 방출된 광만이 핀홀이 설치된 검출기에 의해 검출되어 진다. SPDS를 이용하여 PDP cell 내에서 측정된 3차원 광 intensity 분포로부터 cellso의 방전현상을 다음과 같이 유추해낼수 있었다. Z축 측정이 진행될수록광의 intensity는 증가하였고 ITO전극의 안쪽부분에서 검출되는 광의 intensity가 가장 컸고 Y축 scan시 나타나는 X-Z평면에서 광의 intensity가 격벽과 격벽의 중심부분에서 가장 크게 나타났다.

• 한국입자에어로졸학회지
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• 제4권1호
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• pp.9-20
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• 2008

The effect of light intensity on the ozone formation and the aerosol number concentration during the photochemical reactions of ambient air was investigated in an indoor smog chamber. The smog chamber consists of a housing, 64 blacklights, and a $2.5-m^3$ reaction bag made of Teflon film. The bag was filled with the unfiltered ambient air in Seoul from January 10 to March 18, 2002. In this work, the photolysis rate of $NO_2$, $k_1$ was used as an index of light intensity. Three levels of light intensity were controlled by changing the number of blacklights turned on among 64 blacklights: $0.29min^{-1}$ (50%), $0.44min^{-1}$ (75%), $0.57min^{-1}$ (100%). The ozone concentration increased rapidly within 10 minutes after irradiation irrespective of light intensity, thereafter it increased linearly during the irradiation. The ozone production rate seems to be dependent on both the light intensity and the quality of ambient air introduced into the reaction bag. The change in aerosol number concentration also depended on both the light intensity and the ambient air quality, especially aerosol size distribution. Based on the initial ambient aerosol size distributions, the photochemical potential for aerosol formation and growth is classified into two cases. One is the case showing aerosol formation and growth processes, and the other is the case showing no apparent change in particle size distribution.