• 한국지능시스템학회논문지
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• 제20권3호
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• pp.434-440
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• 2010

In this paper, we define generalized induced linguistic aggregation operator called generalized induced linguistic ordered weighted harmonic mean(GILOWHM) operator. Each object processed by this operator consists of three components, where the first component represents the importance degree or character of the second component, and the second component isused to induce an ordering, through the first component, over the third components which are linguistic variables and then aggregated. It is shown that the induced linguistic ordered weighted harmonic mean(ILOWHM) operator and linguistic ordered weighted harmonic mean(LOWHM) operator are the special cases of the GILOWHM operator. Based on the GILOWHM and LWHM operators, we develop an approach to group decision making with linguistic preference relations. Finally, a numerical example is used to illustrate the applicability of the proposed approach.

• 전자공학회논문지D
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• 제35D권8호
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• pp.62-68
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• 1998

Optical broadband second harmonic genration (SHG) in thin film waveguide structure was investigated. The copolymer poly(MMA-co-DR1MA) which was consiste dof PMMA (polymethylmethacrylate) and DR 1 (disperse red 1) was spin coated on the pyrex substrate. The green and near UV SHG were observe dfrom the fundamental beam even though the poled polymer has the absorption in second harmonic wavelength range. It was able to genrate SHG by cerenkov type phase matching. Th epoled polymer film thickness was decided by theoretical analysis. The green (532nm) and near UV SHG (370nm) were observed from the Q-switched Nd-YAG laser (1064nm) and Ti-sapphire laser (740nm). It was in good agreement with the experimental results.

• The Korean Journal of Ceramics
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• 제6권3호
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• pp.206-208
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• 2000

0.65 mol% MgO-doped LiNbO$_3$single crystals were grown by CZ method. The obtained single crystals were colorless and transparent. Noncritically phase-matched second harmonic generation (SHG) of 532-nm radiation from 1064-nm in MgO-doped LiNbO$_3$has been investigated by using pulsed Nd:YAG laser. The phase-matching temperature was room temperature. SHG conversion efficiencies were typically achieved higher than 50% at the phase-matching temperature with no photorefractive damage in the region of fundamental power density which was used in this experiment. The thermo-birefringence coefficient and the electro-birefringence coefficient of SHG were calculated from the temperature phase-matching profile with the electric field.

• 한국광학회지
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• 제10권4호
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• pp.301-305
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• 1999

Czocharlski pulling method에 의해 성장된 새로운 광학결정 YCOB($YCa_4O(BO_3)_3$)의 파장에 따른 위상 정합 조건을 제시하였으며, Nd:YAG 레이저의 1064nm의 출력을 기본파로 하였을 때 제2조화파 발생 효율을 조사하였다. 또한 $Yb^{3+}$이온과 $Nd^{3+}$ 이온이 도핑된 YCOB의 제2조화파 발생효율을 조사하여 희토류 이온 도핑에 따른 비선형성의 변화를 조사하였다.

• 자연과학논문집
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• 제12권1호
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• pp.31-39
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• 2002

전류밀도와 에칭시간을 변화시키면서 제작된 다공질 규소 초격자의 표면에서 Nd:YAG 레이저의 제2 고조파를 발생시켰다. 이로부터 대칭구조가 바뀌고 유전율이 상승됨이 관측되었다.

• Journal of electromagnetic engineering and science
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• 제5권2호
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• pp.92-96
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• 2005

This paper presents a novel microwave oscillator incorporating a simple microstrip ring type resonant cell as its terminating resonance component. Reduced chip size, higher dc-ac power efficiency, superior harmonic characteristics can be achieved from the introduction of a compact microstrip ring resonator cell. The oscillator provides a second harmonic suppression of 26.51 dB and the output power of 2.046 dBm at 2.11 GHz.

• 한국수학사학회지
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• 제18권1호
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• pp.85-92
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• 2005

본 연구는 변분법과 조화사상 사이에 잘 알려진 내용을 개관하고, 조화사상의 성질 및 발전 과정을 정리하고, 구면 위의 라플라스 작용소의 기본 성질을 정리하고, 구면 사이의 고유함수 사상을 구성하기 위하여 스펙트럼과 고유함수를 계산하였다.

• Current Optics and Photonics
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• 제6권6호
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• pp.576-582
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• 2022

Plasmonic high-order harmonic generation (HHG) is used in nanoscale optical applications because it can help in realizing a compact coherent ultrashort pulse generator on the nanoscale, using plasmonic field enhancement. The plasmonic amplification of nanostructures induces nonlinear optical phenomena such as second-order harmonic generation, third-order harmonic generation, frequency mixing, and HHG. This amplification also causes damage to the structure itself. In this study, the plasmonic amplification according to the design of a metal-coated sapphire conical structure is theoretically calculated, and we analyze the effects of this optical amplification on HHG and damage to the sample.

• 한국정보통신학회논문지
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• 제13권6호
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• pp.1141-1149
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• 2009

Pulse 펄스형 Nd:YAG 레이저는 피부재생치료에 적합하고, 램프에 의해서 연속발진은 물론 정상발진, Q-스위치 및 모드동기 발진까지 다양한 발전 형태가 가능하며 미세수술 및 피부재생 촉진에 널리 사용되어지고 있다. 치료목적에 따라 에너지 밀도를 제어하는 것이 매우 중요하다. 에너지 밀도의 제어는 레이저 출력의 펄스반복률을 제어하는 방법이 주로 사용된다. 본 연구에서는 펄스형 Nd:YAG 레이저의 펄스반복률을 제어할 수 있는 제 2고조파 발생(second harmonic generation: SHG)로 각주파수인 광파의 에너지 일부가 비선형 결정안을 전파하면서 각주파수인 광파의 에너지로 변환되는 현상을 적용하여 2차 비선형성에 의한 제2고조파 발생을 통해 피부심부까지 치료 가능하다는 것은 간단히 관찰할 수 있었다.

• Macromolecular Research
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• 제12권6호
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• pp.581-585
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• 2004

A copolymer P[OSA-MI] was synthesized by copolymerization of its corresponding monomers, N-phenyl maleimide (MI) and 2-octen-l-ylsuccinic anhydride (OSA). The polymer (poly[2-[1-(2,5-dioxo-l-phenylpyrroli­din-3-ylmethyl)heptyl]-succinic acid 4-(2-$\{$ethyl-[4-(4-nitrophen-ylazo)phenyl]amino$\}$ethyl)ester]) P[DR1MA-MI] was obtained from the reaction of P[OSA-MI] with 2-[4-(4-nitrophenylazo)-N-ethylphenylamino] ethanol (DR1). A stable monolayer of P[DRIMA-MI] was formed by spreading the solution of the polymer in chloroform. In Y-type Langmuir-Blodgett (LB) films prepared using this Langmuir-Blodgett method, the second harmonic waves generated from adjacent mono layers canceled each other out. In X-and Z-type LB films, the second harmonic intensity increased upon increasing the number of monolayers, but this increase was somewhat smaller than predicted by the square law. This phenomenon is due to defects or imperfect alignment of the dipoles in the LB film. The generation of second harmonic waves from Y-type LB films having an even number of mono layers supports this argument. The degree of imperfection seemed to increase as the number of layers increased. The second-order nonlinear optical properties of spin-cast films of these polymers were also measured. The largest second harmonic coefficient of the poled P[DRIMA-MI] film coated on a glass plate was 19 pm/V.