• Title/Summary/Keyword: Optimum Wavelength

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Optimum Concentration of the Cd(II)-Quercetin Complexation Reaction (Quercetin의 카드뮴 착물반응에 대한 최적농도)

  • Lee, Jeong-Ho;Shin, Sun-Woo;Baek, Seung-Hwa
    • YAKHAK HOEJI
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    • v.53 no.5
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    • pp.235-240
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    • 2009
  • The interaction of cadmium (II) ion with quercetin was investigated in aqueous solution at different pH. The quercetin/cadmium stochiometries for cadmium (II) binding have been determined by UV-vis spectrophotometric method. The complexation of Cd(II) ion with 54.72 ${\mu}M$ quercetin (A=1.00793) was formed in 0.2 M $NH_3-0.2$ M $NH_4Cl$ (pH 8.0) buffer solution. 1:1 Cd(II)-complex had a maximum absorbance and showed the bathochromic shift of the long-wavelength band of the UV-vis spectra in the alkaline pH when interacted with quercetin in buffer solution. These results suggest that Cd(II)-quercetin complex has the optimal condition of chelation in basic buffer solution.

A Study on HEMT Device Process (Part I. Lift-off Process for the Metallization) (HEMT 소자 공정 연구 (Part 1. 금속박막 형성을 위한 Lift-off 공정연구))

  • 이종람;박성호;김진섭;마동성
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.26 no.10
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    • pp.1535-1544
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    • 1989
  • The overhang structure of photoresist in optical lithography was studied for the metallization of GaAs-related devices throughout lift-off method. Optical contact aligner with a dose of 8.5 m J/cm\ulcornerand with a wavelength of 300mm was used for ultraviolet exposure of single layer of S1400-27 photoresist. The overhang thickness shows a linear relationship with the soaking time in monochlorobenzene, which its magnitude becomes high at elevated softbake temperature. Such process conditions as a low softbake temperature, a long monochlorohbenzene soaking time and a little exposed energy make the development rate of photoresist lower. The optimum process conditions to obtain a target line-width, which include an appropriate overhang structure such as complete separation between the sidewall of photoresist pattern and the deposited metal edge, are determined as the softbake temperature of 64-74\ulcornerC, the monochlorobenzene soaking time of 10-15min, the ultraviolet exposure time of 70-100sec and the development time of 50-80sec.

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Crystal Growth of Er:YAG and Er,Cr:YSGG for Medical Lasers

  • Yu, Young-Moon;Jeoung, Suk-Jong
    • Proceedings of the Korea Association of Crystal Growth Conference
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    • 1998.06a
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    • pp.161-164
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    • 1998
  • Erbium doped garnet crystals were grown by Czochralski method. Relationshipes between crystal quality and crystal growth factors such as pulling rate, rotation rate and concentration of active ions and sensitizers were investigated. Optimum pulling and rotation rate for high quality Er:YAG crystal were 1 mm/hr and 20 rpm and for Er,Cr:YSGG crystal 2-4 mm/hr and 10 rpm respectively. The size of the crystals grown was up to 20-30 mm in diameters and 95-135 mm in length. Er:YAG crystal grown under the nitrogen atmosphere was pink and transparent and Er,Cr:YSGG under the 98% {{{{ { N}_{ 2} }}}} and 2% {{{{ { O}_{2 } }}}} was dark green and transparent. Under the polarizing microscopic observations with crossed polar, striations and {211} core facets were detected. Spectroscopic properties for Er,Cr:YSGG laser rods with <111> axis, 80 mm in length and 6.3 mm in diameter for medical laser applications of 2.79 ${\mu}$m wavelength were manufactured and then laser oscillation was achieved.

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Measurement Guideline of Fresnel-Field Antenna Measurement Method

  • Oh, Soon-Soo;Moon, Jung-Ick
    • ETRI Journal
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    • v.31 no.1
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    • pp.68-70
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    • 2009
  • In this letter, a parametric analysis of the Fresnel-field antenna measurement method is performed for a square aperture. As a result, the optimum number of Fresnel fields for one far-field point is guided as $M_{opt}=N_{opt}=D^2/{\lambda}R+5$, where D is the antenna diameter, ${\lambda}$ is the wavelength, and R is the distance between the source antenna and the antenna under test. For the aperture size 5 ${\leq}$ $L_x/{\lambda}$ ${\leq}$ 20, the tolerable distances for gain errors of 0.5 dB and 0.2 dB can be guided as $R_{0.5\;dB}$ ${\approx}$ $1.2Lx/{\lambda}$ and $R_{0.2\;dB}$ ${\approx}$ $2.0L_x/{\lambda}$, where $L_x$ is the lateral length of the square aperture. The tolerable distances for 20 ${\leq}$ $L_x/{\lambda}$ ${\leq}$ 200 are also proposed. This measurement guideline can be fully utilized when performing the Fresnel-field antenna measurement method.

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A Numerical Analysis of the Amplification Properties of the Regenerative Amplifier (재생증폭기의 증폭특성에 관한 수치해석)

  • 김남희;김병태
    • Korean Journal of Optics and Photonics
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    • v.5 no.1
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    • pp.67-73
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    • 1994
  • The simulation code was developed to analyze the amplification properties of the regenerative amplifier, such as gain narrowing, nonlinear effect, and energy saturation. To reduce gain narrowing in the regenerative amplifier, the input pulse with a symmetrical shape and the same center wavelength of the active medium should be amplified in the active medium with a broad fluorescence linewidth. In this respect, Ti:Sapphire with a low nonlinear refractive index, a high saturation fluence, and a broad fluorescence linewidth is the most appropriate medium for the regenerative amplifier. The knowledge and the important parameters were acquired for the optimum design of the regenerative amplifier.

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12%-Cr 강의 C0$_{2}$레이저 표면 경화

  • 김재도
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 1992.04a
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    • pp.84-88
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    • 1992
  • Laser beam hardenling of 12%-Cr steel has been evaluated by using a continuous wave 3 kW CO$\_$2/ laser with a hardening mirror set. Experiment was performed on the optimum hardening condition with a laser power of 2.85kW and travel speed of 10 and 5 m/min. Multi passes have been alsotried to find the hardening characteristics of partly overlapped zone. The black paint to use at high temperature was adopted to increases the absorptivity of laser beam energy with the wavelength of 10.6 .mu. m at the surface of bese metal. The microstructure of the hardened layers was observed by using a light microscopy. SEM and TEM. A fine lamellar martensite formed in the hardened zones exhibits very high Vickers microhardness of 600 Hv, whereas the tempered martesite distributes in the base metal with Vickers microhardness of 240 Hv. It has been found that laser hardening with multi pass showed no significant drop of the hardness between adjacent passes.

A study regarding the reaction of tetracycline solution in a discolored tooth model using hydroxyapatite granules.

  • Yamaguchi, H.;Shamoto, H.;Sugihara, H.;Yamazaki, Y.;Oshima, T.;Kobayashi, K.;Maeda, N.;Arai, T.
    • Proceedings of the KACD Conference
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    • 2001.11a
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    • pp.564.2-564
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    • 2001
  • For the purpose of explaining the mechanism of tooth discoloration caused by tetracycline (TC), a study was conducted by setting up the following in vitro system. Being evaluated were the TC concentration to give an optimum reaction state when it acted on hydroxyapatite(HA) granules and the absorbing wavelength of TC that had been irradiated with ultraviolet (UV) rays.(omitted)

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Periodically Poled $KNbO_3$ Crystals for Quasi-Phase-Matching

  • Kim, Joong-Hyun;Lee, Sooseok;Yoon, Choon-Sup
    • Proceedings of the Korea Crystallographic Association Conference
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    • 2002.11a
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    • pp.18-18
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    • 2002
  • Although it was suggested in 1962 that an efficient wavelength conversion could be achieved using ferroelectric crystals of periodic 180° domains, it was not until 1990's that quasi-phase-matching (QPM) became realized, as technology for periodic poling of LiNbO₃ crystals was readily available. Since ferroelectric domain inversion brings about change of the sign of second-order nonlinear susceptibility, periodically poled ferroelectric structures provide an ideal way of achieving QPM for second-harmonic generation and optical parametric oscillation. Periodically poled ferroelectric domains can also be utilized for optical devices, such as Brags electrooptic modulators. fabrication of stable periodic domain structures depends on a number of poling parameters of a ferroelectric crystal, such as coercive field, internal field and electrical conductivity. We present poling kinetics of KNbO₃ crystals, which involve domain nucleation and growth, backswitching, relaxation of internal field. Optimum poling conditions were established by designing a proper wave shape of external field. We demonstrate an efficient second-harmonic generation using QPM in a periodically poled KNbO₃ crystal.

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Selenide Glass Optical Fiber Doped with $Pr^{3+}$ for U-Band Optical Amplifier

  • Chung, Woon-Jin;Seo, Hong-Seok;Park, Bong-Je;Ahn, Joon-Tae;Choi, Yong-Gyu
    • ETRI Journal
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    • v.27 no.4
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    • pp.411-417
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    • 2005
  • $Pr^{3+}-doped$ selenide glass optical fiber, which guarantees single-mode propagation of above at least 1310 nm, has been successfully fabricated using a Ge-Ga-Sb-Se glass system. Thermal properties such as glass transition temperature and viscosity of the glasses have been analyzed to find optimum conditions for fiber drawing. Attenuation loss incorporating the effects of an electronic band gap transition, Rayleigh scattering, and multiphonon absorption has also been theoretically estimated for the Ge-Ga-Sb-Se fiber. A conventional double crucible technique has been applied to fabricate the selenide fiber. The background loss of the fiber was estimated to be approximately 0.64 dB/m at 1650 nm, which can be considered fairly good. When excited at approximately 1470 nm, $Pr^{3+}-doped$ selenide fiber resulted in amplified spontaneous emission and saturation behavior with increasing pump power in a U-band wavelength range of 1625 to 1675 nm.

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Analysis of Fourth Harmonic Conversion of High Intensity Nd Laser Beam in KDP Crystal (KDP결정을 이용한 고강도 Nd 레이저광의 제4 고조파변환 해석)

  • 장용무;김병태;강형부
    • The Transactions of the Korean Institute of Electrical Engineers
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    • v.41 no.5
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    • pp.541-550
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    • 1992
  • The fourth harmonic conversion(FHC) efficiency of high-power Nd laser pulse with wavelength of 1.054x10S0-6Tm using two KDP crystals(doubler adn quadrupler) was simulated numerically. Simulation results show that for the perfect phase-matching condition the FHC efficiency were 60-70% for several hundreds MW/cmS02T class and over 70% for GW/cmS02T class laser pulses. And the overall characteristics of FHC were discussed in terms of effects of input intensity, crystal length, and mismatch angle Δ$\theta$. Optimum method to FHC was type-II doubler & type-I quadrupler KDP crystal because type-II KDP doubler crystal has wide tolerance of acceptance matching-angle.