• 한국진공학회지
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• 제9권4호
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• pp.406-410
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• 2000

Hot-wall epitaxy 방법으로 GaAs (100) 기판 위에 9 $\mu\textrm{m}$의 CdTe (111)을 완충층으로 성장하고 그 위에 in-situ로 $Hg_{1-x}Cd_x$/Te (MCT)박막을 성장하였다. 성장된 MCT박막의 2결정 x-선 요동곡선의 반치폭 값은 125 arcsec이었으며 표면 형상의 roughness는 10 nm의 작고 깨끗한 면을 나타내었다. 성장된 MCT 박막에 대한 광전류 측정으로부터 최대 peak 파장과 cut off 파장은 각각 1.1050 $\mu\textrm{m}$ (1.1220 eV)와 1.2632 $\mu\textrm{m}$ (0.9815 eV)임을 알았다 이 peak 파장은 광전도체의 intrinsic transition에 기인한 band gap에 대응하는 봉우리이다. 이로부터 MCT 박막은 1.0 $\mu\textrm{m}$에서 1.6 $\mu\textrm{m}$의 근적외선 파장 영역을 감지할 수 있는 광전도체용 검출기로 쓰일 수 있음을 알았다.

• 한국조명전기설비학회:학술대회논문집
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• 한국조명전기설비학회 2005년도 춘계학술대회논문집
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• pp.421-425
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• 2005

A distributed FBG temperature sensor system was constructed for the use in protection of electric power system. A F-P wavelength tunable filter is used converting temperature-induced wavelength variations to temporal peak locations. We used Gaussian line-fitted algorithm to alleviate the error caused by quantization and electrical noises. The experimental results showed much better accuracy than the raw peak-detection scheme.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2008년도 추계학술대회A
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• pp.1617-1622
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• 2008

We report a new molecular detection process which measures the changes in the plasmon resonance peaks of periodic Au nanoparticle arrays fabricated using the electron beam lithography. As the Au nanoparticle arrays are modified by the chemical reaction in solutions having various concentrations of a target molecule, both the position and intensity of the plasmon peak change in proportion to the concentration of the target molecule. We expect that the process developed in this work can be employed for fine tuning of the plasmon peak wavelength and also for the optical detection of various kinds of molecules. Moreover, this method may improve the measurement accuracy compared with existing approaches that use only one change (peak wavelength or peak intensity) as a readout value for the molecular detection.

• Applied Science and Convergence Technology
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• 제26권4호
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• pp.91-94
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• 2017

AThe effect of localized surface plasmon on silicon substrates was studied using silver nanoparticles. The nanoparticles were formed by self-arrangement through the surface energy using rapid thermal annealing (RTA) technique after the thin nanolayer of silver was deposited by thermal evaporation. By the theoretical calculation based on Mie scattering and dielectric function of air, indium tin oxide (ITO), and silver, the strong peak of scattering cross section of silver nanoparticles was found at 358 nm for air, and 460 nm for ITO, respectively. Accordingly, the strong suppression of reflectance under the condition of induced light of $30^{\circ}$ occurred at the specific wavelength which is almost in accordance with peak of scattering cross section. When the external quantum efficiency was measured using silicon solar cells with silver nanoparticles, there was small enhancement peak near the 460 nm wavelength in which the light was resonated between silver nanoparticles and ITO.

• 에너지공학
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• 제23권1호
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• pp.1-6
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• 2014

본 에너지 분산 형 미세열량측정에 관한 자료는 에너지 분산 형의 우수한 조작 성을 유지하면서 파장 분산 형과 비슷한 정도의 에너지 분해능을 가질 수 있도록 개선한 것으로 광범위한 에너지의 X선을 검출을 할 수 있다. X선을 검출하기 위해서 이용되는 파장 분산 형은 에너지 분해능이 우수하지만 X선의 파장에 대해 검출 각도를 변화시켜야 하고 검출하고자 하는 특정 X선 종류에 따라 몇 가지의 검출기를 필요로 하고 있다. 그러나 에너지 분산 형의 검출기는 한 개의 검출기로 광범위한 X선을 동시에 검출할 수 있으며 조작 방법도 비교적 용이하다. 그러나 에너지 분산 형은 에너지 분해능이 우수하지 못 하고 또한 인접한 에너지를 갖는 X선은 그 피크가 중첩되어 구별하기가 어려운 경우도 있다. 에너지 분해능은 파장분산 형이 2~20 eV이고 에너지 분산 형은 140~180 eV로 상당한 차이가 있다.

• 한국재료학회지
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• 제17권4호
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• pp.198-202
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• 2007

A new organic light emitting device(OLED) with two peak wavelength(blue and yellow) emission was fabricated using the selective doping in a single fluorescent host , and its electrical and optical characteristics were investigated. The fabricated device showed the luminance and efficiency of 1600 $Cd/m^2$ and 2.4 Im/W under the applied voltage of 10V, respectively. And its electroluminescent spectra had two peak wavelengths of 470nm and 560nm emitting bluish white light. The OLED with dual wavelength emission in this experiment is likely to be developed as a white OLED with simpler fluorescent system than conventional devices.

• Journal of the Optical Society of Korea
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• 제20권5호
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• pp.601-606
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• 2016

In this study, in order to analyze the low-temperature sintering process of silver and copper nanoparticles, we calculate their melting temperatures and surface melting temperatures with respect to particle size. For this calculation, we introduce the concept of mean-squared displacement of the atom proposed by Shi (1994). Using a parameter defined by the vibrational component of melting entropy, we readily obtained the surface and bulk melting temperatures of copper and silver nanoparticles. We also calculated the absorption cross-section of nanoparticles for variation in the wavelength of light. By using the calculated absorption cross-section of the nanoparticles at the melting temperature, we obtained the laser threshold energy for the sintering process with respect to particle size and wavelength of laser. We found that the absorption cross-section of silver nanoparticles has a resonant peak at a wavelength of close to 350 nm, yielding the lowest threshold energy. We calculated the intensity distribution around the nanoparticles using the finite-difference time-domain method and confirmed the resonant excitation of silver nanoparticles near the wavelength of the resonant peak.

• Bulletin of the Korean Chemical Society
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• 제35권3호
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• pp.895-898
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• 2014

The wavelength dependence of the photoacoustic signal for n-type GaAs semiconductors in the region of the band-gap energies was investigated. The significant changes in the phase and amplitude of the photoacoustic signal near the band-gap absorption wavelengths were observed to occur when the Si-doping densities in GaAs were varied. Particularly, the first derivatives of the photoacoustic phase vs. wavelength graphs were evaluated and fitted with single Gaussian functions. The peak centers and the widths of the Gaussian curves clearly showed linear relationships with the log values of the Si-doping densities in n-type GaAs semiconductors. It is proposed that the wavelength-dependent PA spectroscopy can be used as a simple and nondestructive method for measuring the doping densities in bulk semiconductors.

• Journal of the Optical Society of Korea
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• 제12권3호
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• pp.157-161
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• 2008

A wavelength-selective reflector, composed of a double-ring-resonator add/drop filter and a loop-back mirror at the drop port to be used for a hybrid-integrated tunable laser is designed and fabricated. High-index-contrast polymer waveguide is used to realize a compact device as small as $2mm{\times}0.4mm$. The radii of the rings are slightly different from each other to obtain a wide wavelength tuning via a vernier effect. Peak reflectivity is measured to be 52% for TE mode and polarization-dependent wavelength shift is 0.95 nm. The tuning range is measured to be about 42 nm for applied current as small as 46 mA.

• 한국가시화정보학회지
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• 제12권3호
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• pp.9-14
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• 2014

Two-photon microscopy (TPM) has been used in plant research as a high-resolution high-depth 3D imaging modality. However, TPM is known to induce photo-damage to the plant in case of long time exposure, and optimal excitation wavelength for plant imaging has not been investigated. Longer excitation wavelength may be appropriate for in vivo two-photon imaging of Arabidopsis thaliana leaves, and effects of longer excitation wavelength were investigated in terms of imaging depth, emission spectrum. Changes of emission spectrum as a function of exposure time at longer excitation wavelength were measured for in vivo longitudinal imaging. Imaging depth was not changed much probably because photon scattering at the cell wall was a limiting factor. Chloroplast emission spectrum showed its intensity peak shift by 20 nm with transition of excitation wavelength from 849 nm or below to 850 nm or higher. Emission spectrum showed different change patterns with excitation wavelengths in longitudinal imaging. Longer excitation wavelengths appeared to interact with chloroplasts differently in comparison with 780 nm excitation wavelength, and may be good for in vivo imaging.